7683:
4167:
4183:
4674:
crystals, the phonon waves are longitudinal or transverse only in certain special symmetry directions. In other directions, they can be nearly longitudinal or nearly transverse. It is only for labeling convenience, that they are often called longitudinal or transverse but are actually quasi-longitudinal or quasi-transverse. Note that in the three-dimensional case, there are two directions perpendicular to a straight line at each point on the line. Hence, there are always two (quasi) transverse waves for each (quasi) longitudinal wave.
5927:
propagation direction is comparable to waves on a string. If the wavelength of acoustic phonons goes to infinity, this corresponds to a simple displacement of the whole crystal, and this costs zero deformation energy. Acoustic phonons exhibit a linear relationship between frequency and phonon wave-vector for long wavelengths. The frequencies of acoustic phonons tend to zero with longer wavelength. Longitudinal and transverse acoustic phonons are often abbreviated as LA and TA phonons, respectively.
9774:
8672:
6316:
4159:
4175:
653:
6015:
2789:
3118:
488:
7241:
7459:
4439:
3403:
641:(i) the total potential energy can be written as a sum of pairwise interactions, and (ii) each atom interacts with only its nearest neighbors. These are used only sparingly in modern lattice dynamics. A more general approach is to express the potential energy in terms of force constants. See, for example, the Wiki article on
4559:, independent of the phonon frequency. As a result, packets of phonons with different (but long) wavelengths can propagate for large distances across the lattice without breaking apart. This is the reason that sound propagates through solids without significant distortion. This behavior fails at large values of
2355:
5741:. Second, each phonon is a "collective mode" caused by the motion of every atom in the lattice. This may be seen from the fact that the creation and annihilation operators, defined here in momentum space, contain sums over the position and momentum operators of every atom when written in position space. (See
2325:
4654:
3p-3 branches will correspond to optical modes. In some special directions, some branches coincide due to symmetry. These branches are called degenerate. In acoustic modes, all the p atoms vibrate in phase. So there is no change in the relative displacements of these atoms during the wave propagation.
2800:
6385:
Thermal phonons can be created and destroyed by random energy fluctuations. In the language of statistical mechanics this means that the chemical potential for adding a phonon is zero. This behavior is an extension of the harmonic potential into the anharmonic regime. The behavior of thermal phonons
4653:
The modes are also referred to as the branches of phonon dispersion. In general, if there are p atoms (denoted by N earlier) in the primitive unit cell, there will be 3p branches of phonon dispersion in a 3-dimensional crystal. Out of these, 3 branches correspond to acoustic modes and the remaining
4669:
The direction of the wave vector is the direction of the wave propagation and the phonon polarization vector gives the direction in which the atoms vibrate. Actually, in general, the wave velocity in a crystal is different for different directions of k. In other words, most crystals are anisotropic
7628:
and negative gravity. This can be explained by how phonons are known to travel faster in denser materials. Because the part of a material pointing towards a gravitational source is closer to the object, it becomes denser on that end. From this, it is predicted that phonons would deflect away as it
7022:
640:
It is important to mention that the mathematical treatment given here is highly simplified in order to make it accessible to non-experts. The simplification has been achieved by making two basic assumptions in the expression for the total potential energy of the crystal. These assumptions are that
4673:
A wave is longitudinal if the atoms vibrate in the same direction as the wave propagation. In a transverse wave, the atoms vibrate perpendicular to the wave propagation. However, except for isotropic crystals, waves in a crystal are not exactly longitudinal or transverse. For general anisotropic
5926:
are coherent movements of atoms of the lattice out of their equilibrium positions. If the displacement is in the direction of propagation, then in some areas the atoms will be closer, in others farther apart, as in a sound wave in air (hence the name acoustic). Displacement perpendicular to the
2059:
477:
The resulting lattice may be visualized as a system of balls connected by springs. The following figure shows a cubic lattice, which is a good model for many types of crystalline solid. Other lattices include a linear chain, which is a very simple lattice which we will shortly use for modeling
6716:
7252:
5903:
4230:
3129:
5059:
6523:
4570:, the dispersion relations exhibit two types of phonons, namely, optical and acoustic modes corresponding to the upper blue and lower red curve in the diagram, respectively. The vertical axis is the energy or frequency of phonon, while the horizontal axis is the
3668:
3526:
6198:
4041:
4933:
5659:
3820:
4688:
differs from the physics of sound in solids, although both are density waves: sound waves in fluids only have longitudinal components, whereas sound waves in solids have longitudinal and transverse components. This is because fluids cannot support
6805:
5495:
1585:
613:
5390:
2784:{\displaystyle {\begin{aligned}\left&=i\hbar \delta _{l,m}\\\left&={\frac {1}{N}}\sum _{l,m}e^{ikal}e^{-ik'am}\left\\&={\frac {i\hbar }{N}}\sum _{l}e^{ial\left(k-k'\right)}=i\hbar \delta _{k,k'}\\\left&=\left=0\end{aligned}}}
713:
Animation showing 6 normal modes of a one-dimensional lattice: a linear chain of particles. The shortest wavelength is at top, with progressively longer wavelengths below. In the lowest lines the motion of the waves to the right can be
438:
are usually imposed. First, the sum is only performed over neighboring atoms. Although the electric forces in real solids extend to infinity, this approximation is still valid because the fields produced by distant atoms are effectively
3946:
3113:{\displaystyle {\begin{aligned}\sum _{l}x_{l}x_{l+m}&={\frac {1}{N}}\sum _{kk'}Q_{k}Q_{k'}\sum _{l}e^{ial\left(k+k'\right)}e^{iamk'}=\sum _{k}Q_{k}Q_{-k}e^{iamk}\\\sum _{l}{p_{l}}^{2}&=\sum _{k}\Pi _{k}\Pi _{-k}\end{aligned}}}
2159:
7236:{\displaystyle {a_{\alpha }}^{\dagger }{\Big |}n_{1}\ldots n_{\alpha -1}n_{\alpha }n_{\alpha +1}\ldots {\Big \rangle }={\sqrt {n_{\alpha }+1}}{\Big |}n_{1}\ldots ,n_{\alpha -1},(n_{\alpha }+1),n_{\alpha +1}\ldots {\Big \rangle }}
6382:. These energy fluctuations are caused by random lattice vibrations, which can be viewed as a gas of phonons. Because these phonons are generated by the temperature of the lattice, they are sometimes designated thermal phonons.
1056:
5952:
center and show no dispersion near that long wavelength limit. This is because they correspond to a mode of vibration where positive and negative ions at adjacent lattice sites swing against each other, creating a time-varying
1890:
6598:
7629:
detects the difference in densities, exhibiting the qualities of a negative gravitational field. Although the effect would be too small to measure, it is possible that future equipment could lead to successful results.
718:
In order to simplify the analysis needed for a 3-dimensional lattice of atoms, it is convenient to model a 1-dimensional lattice or linear chain. This model is complex enough to display the salient features of phonons.
7454:{\displaystyle a_{\alpha }{\Big |}n_{1}\ldots n_{\alpha -1}n_{\alpha }n_{\alpha +1}\ldots {\Big \rangle }={\sqrt {n_{\alpha }}}{\Big |}n_{1}\ldots ,n_{\alpha -1},(n_{\alpha }-1),n_{\alpha +1},\ldots {\Big \rangle }}
5684:
is the occupation number. This can be seen to be a sum of N independent oscillator
Hamiltonians, each with a unique wave vector, and compatible with the methods used for the quantum harmonic oscillator (note that
403:
7556:
727:
The forces between the atoms are assumed to be linear and nearest-neighbour, and they are represented by an elastic spring. Each atom is assumed to be a point particle and the nucleus and electrons move in step
322:
that depends on the distance of separation of the atoms. The potential energy of the entire lattice is the sum of all pairwise potential energies multiplied by a factor of 1/2 to compensate for double counting:
6394:, wherein photons may be emitted or absorbed by the cavity walls. This similarity is not coincidental, for it turns out that the electromagnetic field behaves like a set of harmonic oscillators, giving rise to
6358:
of a crystal. By the nature of this distribution, the heat capacity is dominated by the high-frequency part of the distribution, while thermal conductivity is primarily the result of the low-frequency region.
1447:
5268:
5696:). When a Hamiltonian can be written as a sum of commuting sub-Hamiltonians, the energy eigenstates will be given by the products of eigenstates of each of the separate sub-Hamiltonians. The corresponding
4434:{\displaystyle \omega _{\pm }^{2}=K\left({\frac {1}{m_{1}}}+{\frac {1}{m_{2}}}\right)\pm K{\sqrt {\left({\frac {1}{m_{1}}}+{\frac {1}{m_{2}}}\right)^{2}-{\frac {4\sin ^{2}{\frac {ka}{2}}}{m_{1}m_{2}}}}},}
3398:{\displaystyle {\tfrac {1}{2}}m\omega ^{2}\sum _{j}\left(x_{j}-x_{j+1}\right)^{2}={\tfrac {1}{2}}m\omega ^{2}\sum _{k}Q_{k}Q_{-k}(2-e^{ika}-e^{-ika})={\tfrac {1}{2}}\sum _{k}m{\omega _{k}}^{2}Q_{k}Q_{-k}}
5761:
8552:
Lizée, Mathieu; Marcotte, Alice; Coquinot, Baptiste; Kavokine, Nikita; Sobnath, Karen; Barraud, Clément; Bhardwaj, Ankit; Radha, Boya; Niguès, Antoine; Bocquet, Lydéric; Siria, Alessandro (2023-02-17).
1172:
6350:
properties of a solid are directly related to its phonon structure. The entire set of all possible phonons that are described by the phonon dispersion relations combine in what is known as the phonon
5969:. Optical phonons are often abbreviated as LO and TO phonons, for the longitudinal and transverse modes respectively; the splitting between LO and TO frequencies is often described accurately by the
4938:
1724:
identical atoms. This is the simplest quantum mechanical model of a lattice that allows phonons to arise from it. The formalism for this model is readily generalizable to two and three dimensions.
6408:
5933:
are out-of-phase movements of the atoms in the lattice, one atom moving to the left, and its neighbor to the right. This occurs if the lattice basis consists of two or more atoms. They are called
2805:
2360:
2164:
710:
7671:
They have been also shown to form “phonon winds” where an electric current in a graphene surface is generated by a liquid flow above it due to the viscous forces at the liquid–solid interface.
7561:
The number operator commutes with a string of products of the creation and annihilation operators if and only if the number of creation operators is equal to number of annihilation operators.
5945:, the electric field of the light will move every positive sodium ion in the direction of the field, and every negative chloride ion in the other direction, causing the crystal to vibrate.
4486:
3537:
3414:
2090:
th atom and the sum is made over the nearest neighbors (nn). However one expects that in a lattice there could also appear waves that behave like particles. It is customary to deal with
6082:
3957:
4821:
8209:
6245:
5560:
1706:
3706:
1798:
1247:
6731:
6572:) where, across gaps up to a nanometer wide, heat can flow via phonons that "tunnel" between two materials. This type of heat transfer works between distances too large for
5395:
4755:
1462:
1296:
4657:
Study of phonon dispersion is useful for modeling propagation of sound waves in solids, which is characterized by phonons. The energy of each phonon, as given earlier, is
500:
5293:
1328:
5552:
4809:
2106:
as variables instead of coordinates of particles. The number of normal modes is the same as the number of particles. Still, the
Fourier space is very useful given the
1831:
104:
The study of phonons is an important part of condensed matter physics. They play a major role in many of the physical properties of condensed matter systems, such as
5525:
4782:
1878:
1752:
2320:{\displaystyle {\begin{aligned}Q_{k}&={\frac {1}{\sqrt {N}}}\sum _{l}e^{ikal}x_{l}\\\Pi _{k}&={\frac {1}{\sqrt {N}}}\sum _{l}e^{-ikal}p_{l}.\end{aligned}}}
4098:
All quantum systems show wavelike and particlelike properties simultaneously. The particle-like properties of the phonon are best understood using the methods of
3849:
1851:
6402:: in thermal equilibrium and within the harmonic regime, the probability of finding phonons or photons in a given state with a given angular frequency is:
924:
2054:{\displaystyle {\mathcal {H}}=\sum _{i=1}^{N}{\frac {p_{i}^{2}}{2m}}+{\frac {1}{2}}m\omega ^{2}\sum _{\{ij\}(\mathrm {nn} )}\left(x_{i}-x_{j}\right)^{2}}
7656:
of phonons between the electrons. The evidence that phonons, the vibrations of the ionic lattice, are relevant for superconductivity is provided by the
4150:. This gives rise to the additional normal coordinates, which, as the form of the Hamiltonian indicates, we may view as independent species of phonons.
6711:{\displaystyle {\mathcal {H}}={\tfrac {1}{2}}\sum _{\alpha }\left(p_{\alpha }^{2}+\omega _{\alpha }^{2}q_{\alpha }^{2}-\hbar \omega _{\alpha }\right)}
3700: + 1)th atom as equivalent to the first atom. Physically, this corresponds to joining the chain at its ends. The resulting quantization is
7624:
may have a non-negligible mass and be affected by gravity just as standard particles are. In particular, phonons are predicted to have a kind of
9697:
660:
Due to the connections between atoms, the displacement of one or more atoms from their equilibrium positions gives rise to a set of vibration
8688:
7926:
6308:, and so forth. Physically, the reciprocal lattice vectors act as additional chunks of momentum which the lattice can impart to the phonon.
329:
7496:
5941:, fluctuations in displacement create an electrical polarization that couples to the electromagnetic field. Hence, they can be excited by
4146:. In three dimensions, vibration is not restricted to the direction of propagation, and can also occur in the perpendicular planes, like
1343:
9447:
5898:{\displaystyle {\mathcal {H}}=\sum _{k}\sum _{s=1}^{3}\hbar \,\omega _{k,s}\left({b_{k,s}}^{\dagger }b_{k,s}+{\tfrac {1}{2}}\right).}
9685:
1337:(this requires a significant manipulation using the orthonormality and completeness relations of the discrete Fourier transform),
4142:
of the phonons. In the one-dimensional model, the atoms were restricted to moving along the line, so the phonons corresponded to
1077:
5554:
into the wavevector space
Hamiltonian, as it is defined above, and simplifying then results in the Hamiltonian taking the form:
5074:
4726:
5054:{\displaystyle {b_{k}}^{\dagger }={\sqrt {\frac {m\omega _{k}}{2\hbar }}}\left(Q_{-k}-{\frac {i}{m\omega _{k}}}\Pi _{k}\right)}
4515:
mode. In the optical mode two adjacent different atoms move against each other, while in the acoustic mode they move together.
6518:{\displaystyle n\left(\omega _{k,s}\right)={\frac {1}{\exp \left({\dfrac {\hbar \omega _{k,s}}{k_{\mathrm {B} }T}}\right)-1}}}
8303:
8243:
8190:
8158:
8095:
8063:
8031:
7936:
7909:
7870:
7843:
7807:
7641:
5970:
687:
451:. This is permissible as long as the atoms remain close to their equilibrium positions. Formally, this is accomplished by
8727:
8176:
6722:
5908:
This can be interpreted as the sum of 3N independent oscillator
Hamiltonians, one for each wave vector and polarization.
4812:
8006:
9583:
8133:
7981:
7886:
5976:
When measuring optical phonon energy experimentally, optical phonon frequencies are sometimes given in spectroscopic
3663:{\displaystyle {\mathcal {H}}={\frac {1}{2m}}\sum _{k}\left(\Pi _{k}\Pi _{-k}+m^{2}\omega _{k}^{2}Q_{k}Q_{-k}\right)}
8476:
7482:
annihilates one. Hence, they are respectively the creation and annihilation operators for phonons. Analogous to the
6338:. Additional Brillouin zones may be defined as copies of the first zone, shifted by some reciprocal lattice vector.
3521:{\displaystyle \omega _{k}={\sqrt {2\omega ^{2}\left(1-\cos {ka}\right)}}=2\omega \left|\sin {\frac {ka}{2}}\right|}
9664:
6193:{\displaystyle Q_{k}{\stackrel {\mathrm {def} }{=}}Q_{k+K};\quad \Pi _{k}{\stackrel {\mathrm {def} }{=}}\Pi _{k+K}}
4036:{\displaystyle {\tfrac {1}{2}}\hbar \omega ,\ {\tfrac {3}{2}}\hbar \omega ,\ {\tfrac {5}{2}}\hbar \omega \ \cdots }
7682:
7016:), the phonons are said to be non-interacting. The action of the creation and annihilation operators is given by:
6925:", is the state composed of no phonons. Hence, the energy of the ground state is 0. When a system is in the state
4928:{\displaystyle b_{k}={\sqrt {\frac {m\omega _{k}}{2\hbar }}}\left(Q_{k}+{\frac {i}{m\omega _{k}}}\Pi _{-k}\right)}
4451:
6915:
6811:
4106:
1881:
7732:
8486:
5065:
642:
7860:
5654:{\displaystyle {\mathcal {H}}=\sum _{k}\hbar \omega _{k}\left({b_{k}}^{\dagger }b_{k}+{\tfrac {1}{2}}\right)}
4705:
The above-derived
Hamiltonian may look like a classical Hamiltonian function, but if it is interpreted as an
637:
th atom, which we now measure from its equilibrium position. The sum over nearest neighbors is denoted (nn).
5734:, since any number of identical excitations can be created by repeated application of the creation operator
4087:
must be supplied to the harmonic oscillator lattice to push it to the next energy level. By analogy to the
9680:
8320:
8262:
7742:
6399:
6209:
5664:
This is known as the second quantization technique, also known as the occupation number formulation, where
4678:
4555:(i.e. long wavelengths), the dispersion relation is almost linear, and the speed of sound is approximately
3815:{\displaystyle k=k_{n}={\frac {2\pi n}{Na}}\quad {\mbox{for }}n=0,\pm 1,\pm 2,\ldots \pm {\frac {N}{2}}.\ }
223:
of vibration. Normal modes are important because any arbitrary lattice vibration can be considered to be a
8676:
6870:. Because the difference in energy is what we measure and not the absolute value of it, the constant term
1673:
9808:
7668:
In 2019, researchers were able to isolate individual phonons without destroying them for the first time.
7483:
5742:
4070:
6800:{\displaystyle {\mathcal {H}}=\sum _{\alpha }\hbar \omega _{\alpha }{a_{\alpha }}^{\dagger }a_{\alpha }}
1757:
1203:
7605:
5490:{\displaystyle \Pi _{k}=i{\sqrt {\frac {\hbar m\omega _{k}}{2}}}\left({b_{k}}^{\dagger }-b_{-k}\right)}
2125:
1580:{\displaystyle Q_{k}=A_{k}e^{i\omega _{k}t};\qquad \omega _{k}={\sqrt {{\frac {2C}{m}}(1-\cos {ka})}}.}
1065:
9756:
6867:
608:{\displaystyle \sum _{\{ij\}(\mathrm {nn} )}{\tfrac {1}{2}}m\omega ^{2}\left(R_{i}-R_{j}\right)^{2}.}
244:
168:
6022:(red) do not carry any more information than their counterparts (black) in the first Brillouin zone.
4736:
4567:
9168:
8450:
7487:
5989:
5954:
5385:{\displaystyle Q_{k}={\sqrt {\frac {\hbar }{2m\omega _{k}}}}\left({b_{k}}^{\dagger }+b_{-k}\right)}
1252:
440:
299:
260:
55:
6068:
and integer multiples thereof). For example, in the one-dimensional model, the normal coordinates
434:
explicitly in either classical or quantum mechanics. In order to simplify the task, two important
9798:
9724:
9359:
8986:
8720:
8682:
7609:
5755:
This technique is readily generalized to three dimensions, where the
Hamiltonian takes the form:
5700:
314:
forces are generally negligible. The forces between each pair of atoms may be characterized by a
224:
208:
109:
1301:
9659:
8996:
8694:
6391:
4647:
2349:
This choice retains the desired commutation relations in either real space or wavevector space
693:
Not every possible lattice vibration has a well-defined wavelength and frequency. However, the
136:
82:
8295:
8289:
8051:
7652:
by a weak attractive force. In a conventional superconductor, this attraction is caused by an
5530:
4787:
9746:
8379:
Reiter, D. E.; Sauer, S.; Huneke, J.; Papenkort, T.; Kuhn, T.; Vagov, A.; Axt, V. M. (2009).
8083:
7762:
6031:
5730:
Three important properties of phonons may be deduced from this technique. First, phonons are
4092:
1803:
682:
between atoms. Any wavelength shorter than this can be mapped onto a wavelength longer than 2
668:
of the wave is given by the displacements of the atoms from their equilibrium positions. The
39:
4638: – 3. The lower figure shows the dispersion relations for several phonon modes in
3941:{\displaystyle E_{n}=\left({\tfrac {1}{2}}+n\right)\hbar \omega _{k}\qquad n=0,1,2,3\ldots }
8700:
8633:
8576:
8516:
8396:
8392:
8345:
7772:
7702:
7657:
6395:
5748:
5503:
4760:
4710:
4139:
3692:
The form of the quantization depends on the choice of boundary conditions; for simplicity,
1856:
1730:
1453:
626:
of the harmonic potentials, which are assumed to be the same since the lattice is regular.
105:
43:
8182:
8:
9761:
8744:
8409:
8380:
4718:
4504:
4099:
1709:
1618:
448:
291:
240:
216:
8637:
8580:
8520:
8400:
8349:
686:, due to the periodicity of the lattice. This can be thought of as a consequence of the
664:
propagating through the lattice. One such wave is shown in the figure to the right. The
286:
for a typical sample of a solid. Since the lattice is rigid, the atoms must be exerting
89:
for elastic structures of interacting particles. Phonons can be thought of as quantized
9704:
8713:
8649:
8623:
8592:
8566:
8534:
8361:
8335:
7970:
7880:
7727:
7648:
are expelled from the material. In a superconductor, electrons are bound together into
6573:
6549:
6065:
5942:
5720:
respectively create and destroy a single field excitation, a phonon, with an energy of
4706:
3682:
1836:
113:
79:
8554:
7660:, the dependence of the superconducting critical temperature on the mass of the ions.
4182:
9773:
9741:
9654:
9133:
8878:
8805:
8653:
8596:
8538:
8482:
8299:
8239:
8186:
8154:
8129:
8091:
8059:
8027:
8002:
7977:
7932:
7905:
7866:
7839:
7803:
7722:
7712:
7637:
6577:
6565:
6351:
4627:
4166:
4143:
4066:
1622:
1064:
Since the solutions are expected to be oscillatory, new coordinates are defined by a
1051:{\displaystyle -2Cu_{n}+C\left(u_{n+1}+u_{n-1}\right)=m{\frac {d^{2}u_{n}}{dt^{2}}}.}
729:
623:
479:
431:
200:
86:
24:
8365:
5984:
represents ordinary frequency (not angular frequency), and is expressed in units of
1727:
In contrast to the previous section, the positions of the masses are not denoted by
656:
Phonon propagating through a square lattice (atom displacements greatly exaggerated)
290:
on one another to keep each atom near its equilibrium position. These forces may be
9751:
9522:
9297:
9158:
9143:
8825:
8736:
8641:
8584:
8524:
8507:
8404:
8353:
7747:
6837:
6009:
5966:
5693:
315:
232:
28:
678:
There is a minimum possible wavelength, given by twice the equilibrium separation
9803:
9719:
9644:
9628:
9568:
8978:
8903:
8893:
8883:
8795:
7931:. International publishing locations: Oxford University Press. pp. 231–232.
7717:
6841:
6379:
5938:
4722:
4700:
4631:
4147:
1633:
690:, the lattice points being viewed as the "sampling points" of a continuous wave.
283:
271:
7958:. Solid State Physics. Vol. Supplement 3 (Second ed.). New York: Academic Press.
5992:. In other words, the wave-number in cm units corresponds to the inverse of the
5703:
is then given by the sum of the individual eigenvalues of the sub-Hamiltonians.
3673:
The couplings between the position variables have been transformed away; if the
9778:
9692:
9649:
9385:
9173:
8946:
8868:
8863:
8785:
8645:
8588:
8529:
8502:
7767:
7688:
7645:
6966:
is the occupation number of the phonons. The energy of a single phonon of type
6347:
6334:
6309:
6019:
5949:
4623:
4615:
4548:
4519:
2107:
303:
259:
of quantum mechanics but instead use relations for which there exists a direct
8357:
9792:
9736:
9588:
9555:
9347:
9317:
9249:
9108:
8888:
8815:
8800:
8381:"Generation of squeezed phonon states by optical excitation of a quantum dot"
7737:
7653:
7625:
6581:
6363:
6355:
2095:
452:
435:
295:
132:
75:
67:
4733:
without directly solving the differential equations. Given the
Hamiltonian,
4202:
For a one-dimensional alternating array of two types of ion or atom of mass
9714:
9264:
9254:
9244:
9005:
8956:
8898:
8820:
8775:
8321:"Phonon–phonon interactions due to non-linear effects in a linear ion trap"
7862:
Stalin's great science : the times and adventures of Soviet physicists
7757:
6922:
6367:
4694:
4690:
4522:
in the lattice, is given by the slope of the acoustic dispersion relation,
2099:
709:
120:
8611:
8058:. Physics and Materials Properties (4th ed.). Springer. p. 111.
1597:
represents an independent vibrational mode of the lattice with wavenumber
9729:
9497:
9400:
9395:
9312:
9307:
9237:
9191:
9148:
9113:
9072:
8964:
8928:
8790:
8340:
7649:
6371:
4730:
4563:, i.e. short wavelengths, due to the microscopic details of the lattice.
1602:
694:
267:
220:
98:
90:
8451:"Researchers suggest phonons may have mass and perhaps negative gravity"
6319:
Brillouin zones, (a) in a square lattice, and (b) in a hexagonal lattice
5064:
The following commutators can be easily obtained by substituting in the
9471:
9365:
9355:
9337:
9227:
9128:
9063:
8780:
8705:
8555:"Strong Electronic Winds Blowing under Liquid Flows on Carbon Surfaces"
6387:
6035:
5993:
5985:
5977:
4571:
4121:
4116:
This may be generalized to a three-dimensional lattice. The wavenumber
2343:
2335:
2103:
1626:
798:···o++++++o++++++o++++++o++++++o++++++o++++++o++++++o++++++o++++++o···
669:
3829:
comes from the minimum wavelength, which is twice the lattice spacing
398:{\displaystyle {\frac {1}{2}}\sum _{i\neq j}V\left(r_{i}-r_{j}\right)}
9613:
9603:
9573:
9466:
9432:
9425:
9302:
9292:
9287:
9259:
9027:
8810:
8052:"Fig. 3.2: Phonon dispersion curves in GaAs along high-symmetry axes"
7777:
7551:{\displaystyle N=\sum _{\alpha }{a_{\alpha }}^{\dagger }a_{\alpha }.}
6258:
is thus equivalent to an infinite family of phonons with wavenumbers
5917:
5752:, it can be shown that phonons act as waves of lattice displacement.
698:
665:
307:
212:
204:
180:
146:
124:
6892:
can be ignored without changing the equations of motion. Hence, the
5920:
exhibit two types of phonons: acoustic phonons and optical phonons.
5287:
can be inverted to redefine the conjugate position and momentum as:
4095:
is quantized, the quantum of vibrational energy is called a phonon.
890:
is the distance between atoms when the chain is in equilibrium, and
9709:
9537:
9492:
9476:
9437:
9410:
9123:
9118:
9098:
9068:
9058:
9053:
8873:
8848:
8843:
8770:
8628:
8571:
8437:
8424:
6042:
4158:
2083:
1442:{\displaystyle 2C(\cos {ka-1})Q_{k}=m{\frac {d^{2}Q_{k}}{dt^{2}}}.}
51:
8697:
5957:. Optical phonons that interact in this way with light are called
4518:
The speed of propagation of an acoustic phonon, which is also the
3836:
The harmonic oscillator eigenvalues or energy levels for the mode
282:
is a large number, say of the order of 10, or on the order of the
9618:
9608:
9578:
9532:
9527:
9502:
9420:
9405:
9332:
9327:
9232:
9217:
9163:
9138:
9103:
9032:
9014:
8753:
8671:
8436:
Angelo
Esposito, Rafael Krichevsky, and Alberto Nicolis. (2018).
7707:
7601:
6331:| in their "family". The set of all such wavevectors defines the
6315:
4174:
3685:(which they are not), the transformed Hamiltonian would describe
311:
175:
in the same way that photons represent wave-particle duality for
94:
71:
7564:
It can be shown that phonons are symmetric under exchange (i.e.
4448:
is the wavevector of the vibration related to its wavelength by
1853:
is at its equilibrium position.) In two or more dimensions, the
1720:
A one-dimensional quantum mechanical harmonic chain consists of
1333:
Substitution into the equation of motion produces the following
9593:
9222:
9209:
9200:
9022:
8936:
8835:
7589:
6914:
factor is absent in the operator formalized expression for the
6375:
6027:
5997:
5697:
4088:
4081:
652:
63:
20:
8214:
University of
Cambridge Teaching and Learning Packages Library
6014:
6000:
in vacuum that has the same frequency as the measured phonon.
4811:
defined in the quantum treatment section above, we can define
4701:
Interpretation of phonons using second quantization techniques
9623:
9563:
9415:
9274:
9153:
9093:
9048:
8941:
8919:
8762:
8551:
8084:"§2.1.3 Normal modes of a one-dimensional chain with a basis"
7904:(1st ed.). Oxford: Oxford University Press. p. 82.
7752:
7697:
7621:
5731:
4714:
4685:
4198:) for some waves corresponding to lattice vibrations in GaAs.
2068:
is the mass of each atom (assuming it is equal for all), and
416:
287:
256:
176:
172:
160:
140:
59:
7954:
Maradudin, A.; Montroll, E.; Weiss, G.; Ipatova, I. (1971).
6977:
and the total energy of a general phonon system is given by
470:. The error in ignoring higher order terms remains small if
9390:
9322:
9282:
8858:
8853:
6541:
is the frequency of the phonons (or photons) in the state,
6064:
is only determined up to addition of constant vectors (the
5706:
As with the quantum harmonic oscillator, one can show that
4639:
4170:
Optical and acoustic vibrations in a linear diatomic chain.
2091:
1167:{\displaystyle u_{n}=\sum _{Nak/2\pi =1}^{N}Q_{k}e^{ikna}.}
661:
236:
47:
8378:
8204:
8202:
6814:
in operator formalism, we have not taken into account the
5263:{\displaystyle \left=\delta _{k,k'},\quad {\Big }=\left=0}
4178:
Vibrations of the diatomic chain at different frequencies.
494:
The potential energy of the lattice may now be written as
8481:. Mineola, New York: Dover Publications, Inc. p. 9.
8318:
5988:. The value is obtained by dividing the frequency by the
914:
the mass of the atom, then the equation of motion of the
8319:
Marquet, C.; Schmidt-Kaler, F.; James, D. F. V. (2003).
7956:
Theory of lattice dynamics in the harmonic approximation
6580:
to occur and therefore cannot be explained by classical
6323:
It is usually convenient to consider phonon wavevectors
487:
8199:
458:
about its equilibrium value to quadratic order, giving
211:
of atoms or molecules uniformly oscillates at a single
6613:
6052:
is not actually a physical momentum; it is called the
5876:
5635:
4462:
4010:
3986:
3962:
3872:
3754:
3531:
3329:
3218:
3134:
538:
278:
particles. These particles may be atoms or molecules.
8257:
8255:
7499:
7255:
7025:
6734:
6601:
6459:
6411:
6212:
6085:
5764:
5563:
5533:
5506:
5398:
5296:
5077:
4941:
4824:
4790:
4763:
4739:
4454:
4233:
3960:
3852:
3709:
3540:
3417:
3132:
2803:
2358:
2162:
1893:
1859:
1839:
1806:
1760:
1733:
1676:
1465:
1346:
1304:
1255:
1206:
1080:
927:
503:
332:
302:, and others, all of which are ultimately due to the
7972:
A guide to Feynman Diagrams in the many-body problem
7678:
4677:
Many phonon dispersion curves have been measured by
1800:
as measured from their equilibrium positions. (I.e.
1183:
corresponds and devolves to the continuous variable
8612:"Secret of Flow-Induced Electric Currents Revealed"
8425:
Mutual Interactions of Phonons, Rotons, and Gravity
6374:has an energy that is not constant, but fluctuates
4661:The velocity of the wave also is given in terms of
8693:Phonons in a One Dimensional Microfluidic Crystal
8252:
8119:
8117:
8115:
8113:
8111:
8109:
8107:
7969:
7928:Statistical mechanics: algorithms and computations
7865:. London: Imperial College Press. pp. 64–69.
7550:
7453:
7235:
6799:
6710:
6517:
6370:, and contains no phonons. A lattice at a nonzero
6239:
6192:
5897:
5653:
5546:
5519:
5489:
5384:
5262:
5053:
4927:
4803:
4776:
4749:
4480:
4433:
4035:
3940:
3814:
3662:
3520:
3397:
3112:
2783:
2319:
2053:
1872:
1845:
1825:
1792:
1746:
1700:
1579:
1441:
1322:
1290:
1241:
1166:
1050:
607:
397:
179:. Solids with more than one atom in the smallest
8128:. Saunders College Publishing. pp. 780–783.
7446:
7357:
7333:
7268:
7228:
7142:
7112:
7047:
6048:; however, this is not strictly correct, because
5965:can also interact indirectly with light, through
5948:Optical phonons have a non-zero frequency at the
5190:
5155:
4566:For a crystal that has at least two atoms in its
4491:The connection between frequency and wavevector,
4131:is now associated with three normal coordinates.
188:
184:
119:The concept of phonons was introduced in 1930 by
9790:
7918:
8104:
7999:Theoretical Mechanics of Particles and Continua
7997:Fetter, Alexander; Walecka, John (2003-12-16).
5916:Solids with more than one atom in the smallest
5911:
4697:fluids, which only apply to high frequencies).
4107:Canonical quantization § Real scalar field
3696:boundary conditions are imposed, defining the (
239:phenomena in classical mechanics, phonons have
159:, because long-wavelength phonons give rise to
8503:"Detecting the softest sounds in the Universe"
8123:
7838:. Cambridge University Press. pp. 78–96.
7003: +.... As there are no cross terms (e.g.
163:. The name emphasizes the analogy to the word
8721:
7996:
466:and the elastic force simply proportional to
8423:Alberto Nicolis and Riccardo Penco. (2017).
8238:(3 ed.). India: Elsevier. p. 201.
8233:
8124:Ashcroft, Neil W.; Mermin, N. David (1976).
7829:
7827:
7825:
7823:
7821:
7819:
5500:Directly substituting these definitions for
4481:{\displaystyle k={\tfrac {2\pi }{\lambda }}}
4111:
1992:
1983:
518:
509:
7858:
7620:Recent research has shown that phonons and
6366:temperature, a crystal lattice lies in its
474:remains close to the equilibrium position.
427:is the potential energy between two atoms.
8728:
8714:
8294:. Reading, MA: Benjamin-Cummings. p.
8045:
8043:
7833:
4220:, connected by springs of spring constant
4162:Dispersion curves in linear diatomic chain
1712:, an assembly of independent oscillators.
910:is the elastic constant of the spring and
704:
8627:
8570:
8528:
8408:
8339:
8153:. Princeton: Princeton University Press.
8049:
7816:
7640:is a state of electronic matter in which
5809:
4507:. The plus sign results in the so-called
4102:and operator techniques described later.
2146:defined as the Fourier transforms of the
478:phonons. (For other common lattices, see
255:The equations in this section do not use
8735:
8609:
8427:, Arxiv.org, Retrieved November 27, 2018
8291:Statistical Mechanics, A Set of Lectures
8077:
8075:
6314:
6013:
4181:
4173:
4165:
4157:
708:
697:do possess well-defined wavelengths and
651:
243:properties too, in a way related to the
8474:
8287:
8040:
7967:
7802:(4th ed.). Springer. p. 253.
7797:
7615:
1452:These are the equations for decoupled
903:th atom from its equilibrium position.
9791:
9199:
8495:
8173:
8050:Yu, Peter Y.; Cardona, Manuel (2010).
7924:
4622: ≥ 2 different atoms in the
4153:
722:
16:Quasiparticle of mechanical vibrations
8709:
8385:Journal of Physics: Conference Series
8148:
8142:
8081:
8072:
8021:
7899:
7834:Girvin, Steven M.; Yang, Kun (2019).
6587:
6240:{\displaystyle K={\frac {2n\pi }{a}}}
4757:, as well as the conjugate position,
8015:
7950:
7948:
7632:
7588:), so therefore they are considered
6312:obey a similar set of restrictions.
4216:repeated periodically at a distance
1715:
1701:{\displaystyle \omega (k)\propto ka}
1061:This is a set of coupled equations.
8177:Introduction to Solid State Physics
6921:The ground state, also called the "
6723:creation and annihilation operators
6592:The phonon Hamiltonian is given by
6564:Phonons have been shown to exhibit
6559:
6327:which have the smallest magnitude |
6003:
5937:because in ionic crystals, such as
4813:creation and annihilation operators
4626:exhibits three acoustic modes: one
4120:is replaced by a three-dimensional
250:
13:
6737:
6604:
6489:
6175:
6166:
6163:
6160:
6141:
6112:
6109:
6106:
5767:
5566:
5535:
5400:
5037:
4908:
4792:
4742:
4729:, is a means of extracting energy
4634:. The number of optical modes is 3
3592:
3582:
3543:
3094:
3084:
2752:
2739:
2448:
2240:
2124:may be introduced, defined as the
2002:
1999:
1896:
1793:{\displaystyle x_{1},x_{2},\dots }
1708:. This amounts to classical free
1242:{\displaystyle \phi _{k}=e^{ikna}}
633:is the position coordinate of the
528:
525:
14:
9820:
8664:
8478:Introduction to Superconductivity
7945:
7663:
6755:
6690:
6341:
6034:, phonons have been treated with
5806:
5584:
4986:
4860:
4224:, two modes of vibration result:
4021:
3997:
3973:
3951:The levels are evenly spaced at:
3894:
2660:
2595:
2406:
2086:operators, respectively, for the
462:proportional to the displacement
9772:
9665:Timeline of particle discoveries
8670:
8610:Schirber, Michael (2023-02-17).
7681:
4511:mode, and the minus sign to the
3689:uncoupled harmonic oscillators.
688:Nyquist–Shannon sampling theorem
647:
486:
8603:
8545:
8468:
8443:
8430:
8417:
8372:
8312:
8281:
8227:
8167:
7836:Modern Condensed Matter Physics
7595:
6139:
5152:
3907:
3752:
1515:
8410:10.1088/1742-6596/193/1/012121
8151:Condensed Matter in a Nutshell
8090:. Academic Press. p. 44.
8082:Misra, Prasanta Kumar (2010).
8056:Fundamentals of Semiconductors
7990:
7961:
7893:
7852:
7791:
7416:
7397:
7201:
7182:
6866:terms will add up yielding an
6018:k-vectors exceeding the first
5066:canonical commutation relation
4750:{\displaystyle {\mathcal {H}}}
3322:
3275:
2006:
1995:
1686:
1680:
1569:
1546:
1376:
1353:
1285:
1276:
532:
521:
430:It is difficult to solve this
266:For example: a rigid regular,
1:
8263:"Tunneling across a tiny gap"
8210:"Non-metals: thermal phonons"
7925:Krauth, Werner (April 2006).
7902:The Oxford solid state basics
7885:: CS1 maint: date and year (
7784:
5971:Lyddane–Sachs–Teller relation
3123:The potential energy term is
1291:{\displaystyle k=2\pi j/(Na)}
1068:, in order to decouple them.
643:multiscale Green's functions.
203:description of an elementary
194:
9681:History of subatomic physics
8288:Feynman, Richard P. (1982).
7743:Relativistic heat conduction
5912:Acoustic and optical phonons
4727:quantum harmonic oscillators
4679:inelastic neutron scattering
4642:as a function of wavevector
1187:of scalar field theory. The
167:, in that phonons represent
147:
7:
8515:(7763): 8–9. July 1, 2019.
8440:Retrieved November 11, 2018
8088:Physics of Condensed Matter
7859:Kozhevnikov, A. B. (2004).
7674:
7604:, phonons can interact via
7484:quantum harmonic oscillator
6576:to occur but too small for
6254:. A phonon with wavenumber
5980:notation, where the symbol
5961:. Optical phonons that are
5743:position and momentum space
4071:quantum harmonic oscillator
2126:discrete Fourier transforms
1880:are vector quantities. The
443:. Secondly, the potentials
10:
9825:
8689:Optical and acoustic modes
8646:10.1103/PhysRevX.13.011020
8589:10.1103/PhysRevX.13.011020
8530:10.1038/d41586-019-02009-5
8001:. Dover Books on Physics.
7800:Advanced Quantum Mechanics
7606:parametric down conversion
6066:reciprocal lattice vectors
6007:
5273:Using this, the operators
4721:technique, similar to the
4628:longitudinal acoustic mode
4104:
1323:{\displaystyle j=1\dots N}
1200:for continuum field modes
1066:discrete Fourier transform
882:th atom out of a total of
235:). While normal modes are
141:
112:, as well as in models of
18:
9770:
9673:
9637:
9554:
9515:
9485:
9459:
9455:
9446:
9378:
9346:
9273:
9208:
9190:
9086:
9041:
9013:
9004:
8995:
8977:
8955:
8927:
8918:
8834:
8761:
8752:
8743:
8475:Tinkham, Michael (1996).
8358:10.1007/s00340-003-1097-7
7900:Simon, Steven H. (2013).
7471:creates a phonon of type
4784:, and conjugate momentum
4632:transverse acoustic modes
4112:Three-dimensional lattice
1608:The second equation, for
300:electrostatic attractions
274:) lattice is composed of
9698:mathematical formulation
9293:Eta and eta prime mesons
8174:Kittel, Charles (2004).
7610:squeezed coherent states
7488:particle number operator
6810:Here, in expressing the
6400:Bose–Einstein statistics
5990:speed of light in vacuum
5955:electrical dipole moment
5547:{\displaystyle \Pi _{k}}
4804:{\displaystyle \Pi _{k}}
4684:The physics of sound in
4670:for phonon propagation.
2794:From the general result
1456:which have the solution
899:the displacement of the
263:in classical mechanics.
19:Not to be confused with
9360:Double-charm tetraquark
8234:Pathria; Beale (2011).
7798:Schwabl, Franz (2008).
7464:The creation operator,
4650:of its Brillouin zone.
4614:are those of the first
1826:{\displaystyle x_{i}=0}
1670:, a scalar field, and
1590:Each normal coordinate
705:One-dimensional lattice
151:), which translates to
110:electrical conductivity
8675:Quotations related to
8149:Mahan, Gerald (2010).
8026:. New York: Springer.
7552:
7455:
7237:
6801:
6712:
6519:
6398:. Both gases obey the
6392:electromagnetic cavity
6320:
6241:
6194:
6023:
5899:
5805:
5745:.) Finally, using the
5655:
5548:
5521:
5491:
5386:
5264:
5055:
4929:
4805:
4778:
4751:
4709:, then it describes a
4482:
4435:
4199:
4179:
4171:
4163:
4037:
3942:
3833:, as discussed above.
3816:
3664:
3522:
3399:
3114:
2785:
2321:
2055:
1924:
1874:
1847:
1827:
1794:
1748:
1702:
1601:, which is known as a
1581:
1443:
1324:
1292:
1243:
1168:
1131:
1052:
715:
657:
609:
399:
247:of quantum mechanics.
9757:Wave–particle duality
9747:Relativistic particle
8884:Electron antineutrino
8236:Statistical Mechanics
8024:Many-Particle Physics
8022:Mahan, G. D. (1981).
7763:Surface acoustic wave
7642:electrical resistance
7553:
7456:
7238:
6802:
6725:, these are given by
6713:
6520:
6354:which determines the
6318:
6242:
6195:
6017:
5900:
5785:
5656:
5549:
5522:
5520:{\displaystyle Q_{k}}
5492:
5387:
5265:
5056:
4930:
4806:
4779:
4777:{\displaystyle Q_{k}}
4752:
4574:. The boundaries at −
4483:
4436:
4185:
4177:
4169:
4161:
4093:electromagnetic field
4038:
3943:
3817:
3665:
3523:
3400:
3115:
2786:
2338:of the phonon, i.e. 2
2322:
2117:"normal coordinates"
2082:are the position and
2056:
1904:
1875:
1873:{\displaystyle x_{i}}
1848:
1828:
1795:
1749:
1747:{\displaystyle u_{i}}
1703:
1582:
1444:
1325:
1293:
1244:
1169:
1094:
1053:
712:
655:
610:
400:
245:wave–particle duality
231:vibration modes (cf.
169:wave-particle duality
116:and related effects.
40:collective excitation
8987:Faddeev–Popov ghosts
8737:Particles in physics
8393:Institute of Physics
7968:Mattuck, R. (1976).
7773:Thermal conductivity
7703:Brillouin scattering
7616:Predicted properties
7497:
7486:case, we can define
7253:
7023:
6732:
6599:
6556:is the temperature.
6409:
6396:black-body radiation
6210:
6083:
6076:are defined so that
5762:
5749:correlation function
5561:
5531:
5504:
5396:
5294:
5075:
4939:
4822:
4788:
4761:
4737:
4711:quantum field theory
4648:principal directions
4551:.) At low values of
4452:
4231:
4186:Dispersion relation
4138:= 1, 2, 3 label the
4127:. Furthermore, each
3958:
3850:
3707:
3538:
3415:
3130:
2801:
2356:
2334:turns out to be the
2160:
2139:"conjugate momenta"
1891:
1857:
1837:
1804:
1758:
1731:
1674:
1463:
1454:harmonic oscillators
1344:
1302:
1253:
1204:
1078:
925:
501:
330:
292:Van der Waals forces
135:. It comes from the
106:thermal conductivity
9762:Particle chauvinism
9705:Subatomic particles
8638:2023PhRvX..13a1020L
8581:2023PhRvX..13a1020L
8521:2019Natur.571....8.
8401:2009JPhCS.193a2121R
8350:2003ApPhB..76..199M
8126:Solid State Physics
6948:, we say there are
6686:
6671:
6653:
6041:as though it has a
4719:second quantization
4713:of non-interacting
4505:dispersion relation
4248:
4154:Dispersion relation
4100:second quantization
3825:The upper bound to
3631:
1941:
1884:for this system is
1710:scalar field theory
1619:dispersion relation
1335:decoupled equations
723:Classical treatment
449:harmonic potentials
217:classical mechanics
87:modes of vibrations
9809:1932 introductions
8683:Explained: Phonons
8181:. Wiley. pp.
7728:Carrier scattering
7548:
7515:
7451:
7233:
6797:
6754:
6708:
6672:
6657:
6639:
6633:
6622:
6588:Operator formalism
6550:Boltzmann constant
6515:
6500:
6386:is similar to the
6321:
6237:
6190:
6060:. This is because
6024:
5943:infrared radiation
5895:
5885:
5784:
5747:position–position
5651:
5644:
5583:
5544:
5517:
5487:
5392: and
5382:
5260:
5051:
4935: and
4925:
4801:
4774:
4747:
4478:
4476:
4431:
4234:
4200:
4180:
4172:
4164:
4144:longitudinal waves
4033:
4019:
3995:
3971:
3938:
3881:
3812:
3758:
3660:
3617:
3575:
3518:
3395:
3349:
3338:
3251:
3227:
3167:
3143:
3110:
3108:
3082:
3046:
2990:
2913:
2878:
2817:
2781:
2779:
2613:
2499:
2317:
2315:
2277:
2205:
2051:
2010:
1927:
1870:
1843:
1823:
1790:
1744:
1698:
1617:, is known as the
1577:
1439:
1320:
1288:
1239:
1198:normal coordinates
1164:
1048:
716:
658:
605:
547:
536:
395:
358:
219:this designates a
207:motion in which a
201:quantum mechanical
114:neutron scattering
80:quantum mechanical
58:, specifically in
9786:
9785:
9742:Massless particle
9550:
9549:
9546:
9545:
9511:
9510:
9374:
9373:
9186:
9185:
9182:
9181:
9134:Magnetic monopole
9082:
9081:
8973:
8972:
8914:
8913:
8894:Muon antineutrino
8879:Electron neutrino
8685:, MIT News, 2010.
8559:Physical Review X
8438:The mass of sound
8328:Applied Physics B
8305:978-0-8053-2508-9
8245:978-93-80931-89-0
8192:978-0-471-41526-8
8160:978-0-691-14016-2
8097:978-0-12-384954-0
8065:978-3-642-00709-5
8033:978-0-306-46338-9
7938:978-0-19-851536-4
7911:978-0-19-968077-1
7872:978-1-86094-419-2
7845:978-1-107-13739-4
7809:978-3-540-85062-5
7723:Phonon scattering
7713:Linear elasticity
7638:Superconductivity
7633:Superconductivity
7506:
7353:
7138:
6836:term as, given a
6745:
6624:
6621:
6566:quantum tunneling
6513:
6499:
6352:density of states
6235:
6171:
6117:
5884:
5775:
5643:
5574:
5440:
5439:
5335:
5334:
5034:
4991:
4990:
4905:
4865:
4864:
4618:. A crystal with
4503:), is known as a
4475:
4426:
4424:
4399:
4351:
4331:
4295:
4275:
4067:zero-point energy
4029:
4018:
4008:
3994:
3984:
3970:
3880:
3811:
3804:
3757:
3750:
3566:
3564:
3511:
3476:
3340:
3337:
3242:
3226:
3158:
3142:
3073:
3037:
2981:
2904:
2861:
2859:
2808:
2604:
2602:
2484:
2482:
2268:
2266:
2265:
2196:
2194:
2193:
1978:
1963:
1950:
1846:{\displaystyle i}
1754:, but instead by
1716:Quantum treatment
1623:angular frequency
1572:
1544:
1434:
1196:are known as the
1043:
730:adiabatic theorem
624:natural frequency
546:
504:
480:crystal structure
432:many-body problem
343:
341:
131:was suggested by
74:, a phonon is an
25:Phonon (software)
9816:
9776:
9752:Virtual particle
9523:Mesonic molecule
9457:
9456:
9453:
9452:
9298:Bottom eta meson
9206:
9205:
9197:
9196:
9169:W′ and Z′ bosons
9159:Sterile neutrino
9144:Majorana fermion
9011:
9010:
9002:
9001:
8925:
8924:
8904:Tau antineutrino
8759:
8758:
8750:
8749:
8730:
8723:
8716:
8707:
8706:
8674:
8658:
8657:
8631:
8607:
8601:
8600:
8574:
8549:
8543:
8542:
8532:
8499:
8493:
8492:
8472:
8466:
8465:
8463:
8461:
8447:
8441:
8434:
8428:
8421:
8415:
8414:
8412:
8376:
8370:
8369:
8343:
8341:quant-ph/0211079
8325:
8316:
8310:
8309:
8285:
8279:
8278:
8276:
8274:
8259:
8250:
8249:
8231:
8225:
8224:
8222:
8220:
8206:
8197:
8196:
8171:
8165:
8164:
8146:
8140:
8139:
8121:
8102:
8101:
8079:
8070:
8069:
8047:
8038:
8037:
8019:
8013:
8012:
7994:
7988:
7987:
7975:
7965:
7959:
7952:
7943:
7942:
7922:
7916:
7915:
7897:
7891:
7890:
7884:
7876:
7856:
7850:
7849:
7831:
7814:
7813:
7795:
7748:Rigid unit modes
7733:Phononic crystal
7691:
7686:
7685:
7587:
7575:
7557:
7555:
7554:
7549:
7544:
7543:
7534:
7533:
7528:
7527:
7526:
7514:
7460:
7458:
7457:
7452:
7450:
7449:
7437:
7436:
7409:
7408:
7393:
7392:
7371:
7370:
7361:
7360:
7354:
7352:
7351:
7342:
7337:
7336:
7327:
7326:
7311:
7310:
7301:
7300:
7282:
7281:
7272:
7271:
7265:
7264:
7242:
7240:
7239:
7234:
7232:
7231:
7222:
7221:
7194:
7193:
7178:
7177:
7156:
7155:
7146:
7145:
7139:
7131:
7130:
7121:
7116:
7115:
7106:
7105:
7090:
7089:
7080:
7079:
7061:
7060:
7051:
7050:
7044:
7043:
7038:
7037:
7036:
6955:phonons of type
6947:
6907:
6905:
6904:
6901:
6898:
6885:
6883:
6882:
6879:
6876:
6859:
6857:
6856:
6853:
6850:
6842:infinite lattice
6829:
6827:
6826:
6823:
6820:
6806:
6804:
6803:
6798:
6796:
6795:
6786:
6785:
6780:
6779:
6778:
6767:
6766:
6753:
6741:
6740:
6721:In terms of the
6717:
6715:
6714:
6709:
6707:
6703:
6702:
6701:
6685:
6680:
6670:
6665:
6652:
6647:
6632:
6623:
6614:
6608:
6607:
6570:phonon tunneling
6560:Phonon tunneling
6524:
6522:
6521:
6516:
6514:
6512:
6505:
6501:
6498:
6494:
6493:
6492:
6481:
6480:
6479:
6460:
6443:
6438:
6434:
6433:
6307:
6305:
6304:
6299:
6296:
6295:
6282:
6280:
6279:
6274:
6271:
6270:
6250:for any integer
6246:
6244:
6243:
6238:
6236:
6231:
6220:
6199:
6197:
6196:
6191:
6189:
6188:
6173:
6172:
6170:
6169:
6157:
6152:
6149:
6148:
6135:
6134:
6119:
6118:
6116:
6115:
6103:
6098:
6095:
6094:
6054:crystal momentum
6010:Crystal momentum
6004:Crystal momentum
5967:Raman scattering
5924:Acoustic phonons
5904:
5902:
5901:
5896:
5891:
5887:
5886:
5877:
5871:
5870:
5855:
5854:
5849:
5848:
5847:
5825:
5824:
5804:
5799:
5783:
5771:
5770:
5660:
5658:
5657:
5652:
5650:
5646:
5645:
5636:
5630:
5629:
5620:
5619:
5614:
5613:
5612:
5596:
5595:
5582:
5570:
5569:
5553:
5551:
5550:
5545:
5543:
5542:
5526:
5524:
5523:
5518:
5516:
5515:
5496:
5494:
5493:
5488:
5486:
5482:
5481:
5480:
5465:
5464:
5459:
5458:
5457:
5441:
5435:
5434:
5433:
5417:
5416:
5408:
5407:
5391:
5389:
5388:
5383:
5381:
5377:
5376:
5375:
5360:
5359:
5354:
5353:
5352:
5336:
5333:
5332:
5331:
5312:
5311:
5306:
5305:
5269:
5267:
5266:
5261:
5253:
5249:
5248:
5247:
5242:
5241:
5240:
5239:
5221:
5220:
5215:
5214:
5213:
5194:
5193:
5187:
5186:
5185:
5169:
5168:
5159:
5158:
5148:
5147:
5146:
5124:
5120:
5119:
5118:
5113:
5112:
5111:
5110:
5092:
5091:
5060:
5058:
5057:
5052:
5050:
5046:
5045:
5044:
5035:
5033:
5032:
5031:
5015:
5010:
5009:
4992:
4989:
4981:
4980:
4979:
4966:
4965:
4960:
4959:
4954:
4953:
4952:
4934:
4932:
4931:
4926:
4924:
4920:
4919:
4918:
4906:
4904:
4903:
4902:
4886:
4881:
4880:
4866:
4863:
4855:
4854:
4853:
4840:
4839:
4834:
4833:
4810:
4808:
4807:
4802:
4800:
4799:
4783:
4781:
4780:
4775:
4773:
4772:
4756:
4754:
4753:
4748:
4746:
4745:
4725:method used for
4613:
4611:
4610:
4605:
4602:
4601:
4593:
4591:
4590:
4585:
4582:
4581:
4546:
4544:
4543:
4537:
4534:
4487:
4485:
4484:
4479:
4477:
4471:
4463:
4440:
4438:
4437:
4432:
4427:
4425:
4423:
4422:
4421:
4412:
4411:
4401:
4400:
4395:
4387:
4382:
4381:
4368:
4363:
4362:
4357:
4353:
4352:
4350:
4349:
4337:
4332:
4330:
4329:
4317:
4309:
4301:
4297:
4296:
4294:
4293:
4281:
4276:
4274:
4273:
4261:
4247:
4242:
4148:transverse waves
4134:The new indices
4061:
4059:
4058:
4055:
4052:
4042:
4040:
4039:
4034:
4027:
4020:
4011:
4006:
3996:
3987:
3982:
3972:
3963:
3947:
3945:
3944:
3939:
3906:
3905:
3893:
3889:
3882:
3873:
3862:
3861:
3821:
3819:
3818:
3813:
3809:
3805:
3797:
3759:
3755:
3751:
3749:
3741:
3730:
3725:
3724:
3669:
3667:
3666:
3661:
3659:
3655:
3654:
3653:
3641:
3640:
3630:
3625:
3616:
3615:
3603:
3602:
3590:
3589:
3574:
3565:
3563:
3552:
3547:
3546:
3527:
3525:
3524:
3519:
3517:
3513:
3512:
3507:
3499:
3477:
3475:
3471:
3470:
3445:
3444:
3432:
3427:
3426:
3404:
3402:
3401:
3396:
3394:
3393:
3381:
3380:
3371:
3370:
3365:
3364:
3363:
3348:
3339:
3330:
3321:
3320:
3299:
3298:
3274:
3273:
3261:
3260:
3250:
3241:
3240:
3228:
3219:
3213:
3212:
3207:
3203:
3202:
3201:
3183:
3182:
3166:
3157:
3156:
3144:
3135:
3119:
3117:
3116:
3111:
3109:
3105:
3104:
3092:
3091:
3081:
3065:
3064:
3059:
3058:
3057:
3045:
3032:
3031:
3013:
3012:
3000:
2999:
2989:
2977:
2976:
2975:
2953:
2952:
2951:
2947:
2946:
2912:
2903:
2902:
2901:
2888:
2887:
2877:
2876:
2860:
2852:
2843:
2842:
2827:
2826:
2816:
2790:
2788:
2787:
2782:
2780:
2770:
2766:
2765:
2764:
2763:
2747:
2746:
2725:
2721:
2720:
2719:
2718:
2702:
2701:
2683:
2682:
2681:
2653:
2652:
2651:
2647:
2646:
2612:
2603:
2598:
2590:
2582:
2578:
2574:
2573:
2572:
2560:
2559:
2545:
2544:
2537:
2518:
2517:
2498:
2483:
2475:
2466:
2462:
2461:
2460:
2459:
2443:
2442:
2424:
2423:
2395:
2391:
2390:
2389:
2377:
2376:
2341:
2326:
2324:
2323:
2318:
2316:
2309:
2308:
2299:
2298:
2276:
2267:
2261:
2257:
2248:
2247:
2234:
2233:
2224:
2223:
2204:
2195:
2189:
2185:
2176:
2175:
2060:
2058:
2057:
2052:
2050:
2049:
2044:
2040:
2039:
2038:
2026:
2025:
2009:
2005:
1977:
1976:
1964:
1956:
1951:
1949:
1940:
1935:
1926:
1923:
1918:
1900:
1899:
1879:
1877:
1876:
1871:
1869:
1868:
1852:
1850:
1849:
1844:
1832:
1830:
1829:
1824:
1816:
1815:
1799:
1797:
1796:
1791:
1783:
1782:
1770:
1769:
1753:
1751:
1750:
1745:
1743:
1742:
1707:
1705:
1704:
1699:
1669:
1658:
1649:
1643:
1639:
1616:
1600:
1586:
1584:
1583:
1578:
1573:
1568:
1545:
1540:
1532:
1530:
1525:
1524:
1511:
1510:
1506:
1505:
1488:
1487:
1475:
1474:
1448:
1446:
1445:
1440:
1435:
1433:
1432:
1431:
1418:
1417:
1416:
1407:
1406:
1396:
1388:
1387:
1375:
1329:
1327:
1326:
1321:
1297:
1295:
1294:
1289:
1275:
1248:
1246:
1245:
1240:
1238:
1237:
1216:
1215:
1195:
1186:
1182:
1173:
1171:
1170:
1165:
1160:
1159:
1141:
1140:
1130:
1125:
1112:
1090:
1089:
1057:
1055:
1054:
1049:
1044:
1042:
1041:
1040:
1027:
1026:
1025:
1016:
1015:
1005:
997:
993:
992:
991:
973:
972:
946:
945:
917:
913:
902:
898:
889:
885:
881:
877:
847:
838:
823:
819:
779:
773:
769:
762:
756:
614:
612:
611:
606:
601:
600:
595:
591:
590:
589:
577:
576:
561:
560:
548:
539:
535:
531:
490:
453:Taylor expanding
404:
402:
401:
396:
394:
390:
389:
388:
376:
375:
357:
342:
334:
316:potential energy
251:Lattice dynamics
233:Fourier analysis
199:A phonon is the
150:
144:
143:
56:condensed matter
29:Phonon (company)
9824:
9823:
9819:
9818:
9817:
9815:
9814:
9813:
9789:
9788:
9787:
9782:
9766:
9720:Nuclear physics
9669:
9633:
9569:Davydov soliton
9542:
9507:
9481:
9442:
9370:
9342:
9269:
9178:
9078:
9037:
8991:
8969:
8951:
8910:
8830:
8739:
8734:
8699:with movies in
8667:
8662:
8661:
8608:
8604:
8550:
8546:
8501:
8500:
8496:
8489:
8473:
8469:
8459:
8457:
8449:
8448:
8444:
8435:
8431:
8422:
8418:
8377:
8373:
8323:
8317:
8313:
8306:
8286:
8282:
8272:
8270:
8261:
8260:
8253:
8246:
8232:
8228:
8218:
8216:
8208:
8207:
8200:
8193:
8172:
8168:
8161:
8147:
8143:
8136:
8122:
8105:
8098:
8080:
8073:
8066:
8048:
8041:
8034:
8020:
8016:
8009:
7995:
7991:
7984:
7976:. McGraw-Hill.
7966:
7962:
7953:
7946:
7939:
7923:
7919:
7912:
7898:
7894:
7878:
7877:
7873:
7857:
7853:
7846:
7832:
7817:
7810:
7796:
7792:
7787:
7782:
7718:Mechanical wave
7687:
7680:
7677:
7666:
7646:magnetic fields
7635:
7618:
7598:
7577:
7565:
7539:
7535:
7529:
7522:
7518:
7517:
7516:
7510:
7498:
7495:
7494:
7480:
7469:
7445:
7444:
7426:
7422:
7404:
7400:
7382:
7378:
7366:
7362:
7356:
7355:
7347:
7343:
7341:
7332:
7331:
7316:
7312:
7306:
7302:
7290:
7286:
7277:
7273:
7267:
7266:
7260:
7256:
7254:
7251:
7250:
7227:
7226:
7211:
7207:
7189:
7185:
7167:
7163:
7151:
7147:
7141:
7140:
7126:
7122:
7120:
7111:
7110:
7095:
7091:
7085:
7081:
7069:
7065:
7056:
7052:
7046:
7045:
7039:
7032:
7028:
7027:
7026:
7024:
7021:
7020:
7015:
7009:
7002:
6996:
6989:
6983:
6975:
6964:
6953:
6945:
6939:
6933:
6926:
6912:
6902:
6899:
6896:
6895:
6893:
6890:
6880:
6877:
6874:
6873:
6871:
6864:
6854:
6851:
6848:
6847:
6845:
6834:
6824:
6821:
6818:
6817:
6815:
6791:
6787:
6781:
6774:
6770:
6769:
6768:
6762:
6758:
6749:
6736:
6735:
6733:
6730:
6729:
6697:
6693:
6681:
6676:
6666:
6661:
6648:
6643:
6638:
6634:
6628:
6612:
6603:
6602:
6600:
6597:
6596:
6590:
6562:
6547:
6540:
6488:
6487:
6483:
6482:
6469:
6465:
6461:
6458:
6454:
6447:
6442:
6423:
6419:
6415:
6410:
6407:
6406:
6390:produced by an
6344:
6310:Bloch electrons
6300:
6297:
6293:
6291:
6290:
6288:
6275:
6272:
6268:
6266:
6265:
6263:
6221:
6219:
6211:
6208:
6207:
6178:
6174:
6159:
6158:
6153:
6151:
6150:
6144:
6140:
6124:
6120:
6105:
6104:
6099:
6097:
6096:
6090:
6086:
6084:
6081:
6080:
6012:
6006:
5959:infrared active
5939:sodium chloride
5931:Optical phonons
5914:
5875:
5860:
5856:
5850:
5837:
5833:
5832:
5831:
5830:
5826:
5814:
5810:
5800:
5789:
5779:
5766:
5765:
5763:
5760:
5759:
5739:
5725:
5718:
5711:
5690:
5682:
5676:
5669:
5634:
5625:
5621:
5615:
5608:
5604:
5603:
5602:
5601:
5597:
5591:
5587:
5578:
5565:
5564:
5562:
5559:
5558:
5538:
5534:
5532:
5529:
5528:
5511:
5507:
5505:
5502:
5501:
5473:
5469:
5460:
5453:
5449:
5448:
5447:
5446:
5442:
5429:
5425:
5418:
5415:
5403:
5399:
5397:
5394:
5393:
5368:
5364:
5355:
5348:
5344:
5343:
5342:
5341:
5337:
5327:
5323:
5316:
5310:
5301:
5297:
5295:
5292:
5291:
5285:
5278:
5243:
5232:
5231:
5227:
5226:
5225:
5216:
5209:
5205:
5204:
5203:
5202:
5198:
5189:
5188:
5178:
5177:
5173:
5164:
5160:
5154:
5153:
5139:
5132:
5128:
5114:
5103:
5102:
5098:
5097:
5096:
5087:
5083:
5082:
5078:
5076:
5073:
5072:
5040:
5036:
5027:
5023:
5019:
5014:
5002:
4998:
4997:
4993:
4982:
4975:
4971:
4967:
4964:
4955:
4948:
4944:
4943:
4942:
4940:
4937:
4936:
4911:
4907:
4898:
4894:
4890:
4885:
4876:
4872:
4871:
4867:
4856:
4849:
4845:
4841:
4838:
4829:
4825:
4823:
4820:
4819:
4795:
4791:
4789:
4786:
4785:
4768:
4764:
4762:
4759:
4758:
4741:
4740:
4738:
4735:
4734:
4723:ladder operator
4703:
4606:
4603:
4599:
4598:
4597:
4595:
4586:
4583:
4579:
4578:
4577:
4575:
4538:
4535:
4532:
4526:
4525:
4523:
4464:
4461:
4453:
4450:
4449:
4417:
4413:
4407:
4403:
4402:
4388:
4386:
4377:
4373:
4369:
4367:
4358:
4345:
4341:
4336:
4325:
4321:
4316:
4315:
4311:
4310:
4308:
4289:
4285:
4280:
4269:
4265:
4260:
4259:
4255:
4243:
4238:
4232:
4229:
4228:
4215:
4208:
4156:
4114:
4109:
4056:
4053:
4050:
4049:
4047:
4009:
3985:
3961:
3959:
3956:
3955:
3901:
3897:
3871:
3870:
3866:
3857:
3853:
3851:
3848:
3847:
3841:
3796:
3753:
3742:
3731:
3729:
3720:
3716:
3708:
3705:
3704:
3646:
3642:
3636:
3632:
3626:
3621:
3611:
3607:
3595:
3591:
3585:
3581:
3580:
3576:
3570:
3556:
3551:
3542:
3541:
3539:
3536:
3535:
3500:
3498:
3491:
3487:
3463:
3450:
3446:
3440:
3436:
3431:
3422:
3418:
3416:
3413:
3412:
3386:
3382:
3376:
3372:
3366:
3359:
3355:
3354:
3353:
3344:
3328:
3307:
3303:
3288:
3284:
3266:
3262:
3256:
3252:
3246:
3236:
3232:
3217:
3208:
3191:
3187:
3178:
3174:
3173:
3169:
3168:
3162:
3152:
3148:
3133:
3131:
3128:
3127:
3107:
3106:
3097:
3093:
3087:
3083:
3077:
3066:
3060:
3053:
3049:
3048:
3047:
3041:
3034:
3033:
3018:
3014:
3005:
3001:
2995:
2991:
2985:
2968:
2958:
2954:
2939:
2932:
2928:
2918:
2914:
2908:
2894:
2893:
2889:
2883:
2879:
2869:
2865:
2851:
2844:
2832:
2828:
2822:
2818:
2812:
2804:
2802:
2799:
2798:
2778:
2777:
2756:
2755:
2751:
2742:
2738:
2737:
2733:
2726:
2711:
2710:
2706:
2697:
2693:
2692:
2688:
2685:
2684:
2674:
2667:
2663:
2639:
2632:
2628:
2618:
2614:
2608:
2591:
2589:
2580:
2579:
2568:
2564:
2555:
2551:
2550:
2546:
2530:
2523:
2519:
2504:
2500:
2488:
2474:
2467:
2452:
2451:
2447:
2438:
2434:
2433:
2429:
2426:
2425:
2413:
2409:
2396:
2385:
2381:
2372:
2368:
2367:
2363:
2359:
2357:
2354:
2353:
2342:divided by the
2339:
2314:
2313:
2304:
2300:
2282:
2278:
2272:
2256:
2249:
2243:
2239:
2236:
2235:
2229:
2225:
2210:
2206:
2200:
2184:
2177:
2171:
2167:
2163:
2161:
2158:
2157:
2151:
2144:
2133:
2122:
2110:of the system.
2080:
2073:
2045:
2034:
2030:
2021:
2017:
2016:
2012:
2011:
1998:
1982:
1972:
1968:
1955:
1942:
1936:
1931:
1925:
1919:
1908:
1895:
1894:
1892:
1889:
1888:
1864:
1860:
1858:
1855:
1854:
1838:
1835:
1834:
1811:
1807:
1805:
1802:
1801:
1778:
1774:
1765:
1761:
1759:
1756:
1755:
1738:
1734:
1732:
1729:
1728:
1718:
1675:
1672:
1671:
1660:
1656:
1651:
1645:
1641:
1637:
1634:continuum limit
1614:
1609:
1598:
1595:
1561:
1533:
1531:
1529:
1520:
1516:
1501:
1497:
1493:
1489:
1483:
1479:
1470:
1466:
1464:
1461:
1460:
1427:
1423:
1419:
1412:
1408:
1402:
1398:
1397:
1395:
1383:
1379:
1362:
1345:
1342:
1341:
1303:
1300:
1299:
1271:
1254:
1251:
1250:
1224:
1220:
1211:
1207:
1205:
1202:
1201:
1193:
1188:
1184:
1178:
1146:
1142:
1136:
1132:
1126:
1108:
1098:
1085:
1081:
1079:
1076:
1075:
1036:
1032:
1028:
1021:
1017:
1011:
1007:
1006:
1004:
981:
977:
962:
958:
957:
953:
941:
937:
926:
923:
922:
915:
911:
900:
896:
891:
887:
883:
879:
875:
856:
845:
843:
836:
835:
821:
817:
777:
771:
767:
760:
754:
725:
707:
650:
631:
596:
585:
581:
572:
568:
567:
563:
562:
556:
552:
537:
524:
508:
502:
499:
498:
447:are treated as
413:
384:
380:
371:
367:
366:
362:
347:
333:
331:
328:
327:
284:Avogadro number
253:
197:
46:arrangement of
42:in a periodic,
32:
17:
12:
11:
5:
9822:
9812:
9811:
9806:
9801:
9799:Quasiparticles
9784:
9783:
9779:Physics portal
9771:
9768:
9767:
9765:
9764:
9759:
9754:
9749:
9744:
9739:
9734:
9733:
9732:
9722:
9717:
9712:
9707:
9702:
9701:
9700:
9693:Standard Model
9690:
9689:
9688:
9677:
9675:
9671:
9670:
9668:
9667:
9662:
9660:Quasiparticles
9657:
9652:
9647:
9641:
9639:
9635:
9634:
9632:
9631:
9626:
9621:
9616:
9611:
9606:
9601:
9596:
9591:
9586:
9581:
9576:
9571:
9566:
9560:
9558:
9556:Quasiparticles
9552:
9551:
9548:
9547:
9544:
9543:
9541:
9540:
9535:
9530:
9525:
9519:
9517:
9513:
9512:
9509:
9508:
9506:
9505:
9500:
9495:
9489:
9487:
9483:
9482:
9480:
9479:
9474:
9469:
9463:
9461:
9450:
9444:
9443:
9441:
9440:
9435:
9430:
9429:
9428:
9423:
9418:
9413:
9408:
9403:
9393:
9388:
9382:
9380:
9376:
9375:
9372:
9371:
9369:
9368:
9363:
9352:
9350:
9348:Exotic hadrons
9344:
9343:
9341:
9340:
9335:
9330:
9325:
9320:
9315:
9310:
9305:
9300:
9295:
9290:
9285:
9279:
9277:
9271:
9270:
9268:
9267:
9262:
9257:
9252:
9247:
9242:
9241:
9240:
9235:
9230:
9225:
9214:
9212:
9203:
9194:
9188:
9187:
9184:
9183:
9180:
9179:
9177:
9176:
9174:X and Y bosons
9171:
9166:
9161:
9156:
9151:
9146:
9141:
9136:
9131:
9126:
9121:
9116:
9111:
9106:
9101:
9096:
9090:
9088:
9084:
9083:
9080:
9079:
9077:
9076:
9066:
9061:
9056:
9051:
9045:
9043:
9039:
9038:
9036:
9035:
9030:
9025:
9019:
9017:
9008:
8999:
8993:
8992:
8990:
8989:
8983:
8981:
8975:
8974:
8971:
8970:
8968:
8967:
8961:
8959:
8953:
8952:
8950:
8949:
8947:W and Z bosons
8944:
8939:
8933:
8931:
8922:
8916:
8915:
8912:
8911:
8909:
8908:
8907:
8906:
8901:
8896:
8891:
8886:
8881:
8871:
8866:
8861:
8856:
8851:
8846:
8840:
8838:
8832:
8831:
8829:
8828:
8823:
8818:
8813:
8808:
8803:
8801:Strange (quark
8798:
8793:
8788:
8783:
8778:
8773:
8767:
8765:
8756:
8747:
8741:
8740:
8733:
8732:
8725:
8718:
8710:
8704:
8703:
8691:
8686:
8680:
8666:
8665:External links
8663:
8660:
8659:
8602:
8544:
8494:
8487:
8467:
8442:
8429:
8416:
8371:
8334:(3): 199–208.
8311:
8304:
8280:
8269:. 7 April 2015
8251:
8244:
8226:
8198:
8191:
8166:
8159:
8141:
8134:
8103:
8096:
8071:
8064:
8039:
8032:
8014:
8008:978-0486432618
8007:
7989:
7982:
7960:
7944:
7937:
7917:
7910:
7892:
7871:
7851:
7844:
7815:
7808:
7789:
7788:
7786:
7783:
7781:
7780:
7775:
7770:
7768:Surface phonon
7765:
7760:
7755:
7750:
7745:
7740:
7735:
7730:
7725:
7720:
7715:
7710:
7705:
7700:
7694:
7693:
7692:
7689:Physics portal
7676:
7673:
7665:
7664:Other research
7662:
7658:isotope effect
7634:
7631:
7617:
7614:
7597:
7594:
7559:
7558:
7547:
7542:
7538:
7532:
7525:
7521:
7513:
7509:
7505:
7502:
7478:
7467:
7462:
7461:
7448:
7443:
7440:
7435:
7432:
7429:
7425:
7421:
7418:
7415:
7412:
7407:
7403:
7399:
7396:
7391:
7388:
7385:
7381:
7377:
7374:
7369:
7365:
7359:
7350:
7346:
7340:
7335:
7330:
7325:
7322:
7319:
7315:
7309:
7305:
7299:
7296:
7293:
7289:
7285:
7280:
7276:
7270:
7263:
7259:
7244:
7243:
7230:
7225:
7220:
7217:
7214:
7210:
7206:
7203:
7200:
7197:
7192:
7188:
7184:
7181:
7176:
7173:
7170:
7166:
7162:
7159:
7154:
7150:
7144:
7137:
7134:
7129:
7125:
7119:
7114:
7109:
7104:
7101:
7098:
7094:
7088:
7084:
7078:
7075:
7072:
7068:
7064:
7059:
7055:
7049:
7042:
7035:
7031:
7013:
7007:
7000:
6994:
6987:
6981:
6973:
6962:
6951:
6943:
6937:
6931:
6910:
6888:
6862:
6832:
6808:
6807:
6794:
6790:
6784:
6777:
6773:
6765:
6761:
6757:
6752:
6748:
6744:
6739:
6719:
6718:
6706:
6700:
6696:
6692:
6689:
6684:
6679:
6675:
6669:
6664:
6660:
6656:
6651:
6646:
6642:
6637:
6631:
6627:
6620:
6617:
6611:
6606:
6589:
6586:
6561:
6558:
6545:
6532:
6526:
6525:
6511:
6508:
6504:
6497:
6491:
6486:
6478:
6475:
6472:
6468:
6464:
6457:
6453:
6450:
6446:
6441:
6437:
6432:
6429:
6426:
6422:
6418:
6414:
6343:
6342:Thermodynamics
6340:
6335:Brillouin zone
6248:
6247:
6234:
6230:
6227:
6224:
6218:
6215:
6201:
6200:
6187:
6184:
6181:
6177:
6168:
6165:
6162:
6156:
6147:
6143:
6138:
6133:
6130:
6127:
6123:
6114:
6111:
6108:
6102:
6093:
6089:
6058:pseudomomentum
6026:By analogy to
6020:Brillouin zone
6008:Main article:
6005:
6002:
5950:Brillouin zone
5913:
5910:
5906:
5905:
5894:
5890:
5883:
5880:
5874:
5869:
5866:
5863:
5859:
5853:
5846:
5843:
5840:
5836:
5829:
5823:
5820:
5817:
5813:
5808:
5803:
5798:
5795:
5792:
5788:
5782:
5778:
5774:
5769:
5737:
5723:
5716:
5709:
5688:
5680:
5674:
5667:
5662:
5661:
5649:
5642:
5639:
5633:
5628:
5624:
5618:
5611:
5607:
5600:
5594:
5590:
5586:
5581:
5577:
5573:
5568:
5541:
5537:
5514:
5510:
5498:
5497:
5485:
5479:
5476:
5472:
5468:
5463:
5456:
5452:
5445:
5438:
5432:
5428:
5424:
5421:
5414:
5411:
5406:
5402:
5380:
5374:
5371:
5367:
5363:
5358:
5351:
5347:
5340:
5330:
5326:
5322:
5319:
5315:
5309:
5304:
5300:
5283:
5276:
5271:
5270:
5259:
5256:
5252:
5246:
5238:
5235:
5230:
5224:
5219:
5212:
5208:
5201:
5197:
5192:
5184:
5181:
5176:
5172:
5167:
5163:
5157:
5151:
5145:
5142:
5138:
5135:
5131:
5127:
5123:
5117:
5109:
5106:
5101:
5095:
5090:
5086:
5081:
5062:
5061:
5049:
5043:
5039:
5030:
5026:
5022:
5018:
5013:
5008:
5005:
5001:
4996:
4988:
4985:
4978:
4974:
4970:
4963:
4958:
4951:
4947:
4923:
4917:
4914:
4910:
4901:
4897:
4893:
4889:
4884:
4879:
4875:
4870:
4862:
4859:
4852:
4848:
4844:
4837:
4832:
4828:
4798:
4794:
4771:
4767:
4744:
4702:
4699:
4691:shear stresses
4624:primitive cell
4616:Brillouin zone
4568:primitive cell
4549:group velocity
4530:
4520:speed of sound
4474:
4470:
4467:
4460:
4457:
4442:
4441:
4430:
4420:
4416:
4410:
4406:
4398:
4394:
4391:
4385:
4380:
4376:
4372:
4366:
4361:
4356:
4348:
4344:
4340:
4335:
4328:
4324:
4320:
4314:
4307:
4304:
4300:
4292:
4288:
4284:
4279:
4272:
4268:
4264:
4258:
4254:
4251:
4246:
4241:
4237:
4213:
4206:
4155:
4152:
4113:
4110:
4091:case when the
4044:
4043:
4032:
4026:
4023:
4017:
4014:
4005:
4002:
3999:
3993:
3990:
3981:
3978:
3975:
3969:
3966:
3949:
3948:
3937:
3934:
3931:
3928:
3925:
3922:
3919:
3916:
3913:
3910:
3904:
3900:
3896:
3892:
3888:
3885:
3879:
3876:
3869:
3865:
3860:
3856:
3839:
3823:
3822:
3808:
3803:
3800:
3795:
3792:
3789:
3786:
3783:
3780:
3777:
3774:
3771:
3768:
3765:
3762:
3748:
3745:
3740:
3737:
3734:
3728:
3723:
3719:
3715:
3712:
3671:
3670:
3658:
3652:
3649:
3645:
3639:
3635:
3629:
3624:
3620:
3614:
3610:
3606:
3601:
3598:
3594:
3588:
3584:
3579:
3573:
3569:
3562:
3559:
3555:
3550:
3545:
3529:
3528:
3516:
3510:
3506:
3503:
3497:
3494:
3490:
3486:
3483:
3480:
3474:
3469:
3466:
3462:
3459:
3456:
3453:
3449:
3443:
3439:
3435:
3430:
3425:
3421:
3406:
3405:
3392:
3389:
3385:
3379:
3375:
3369:
3362:
3358:
3352:
3347:
3343:
3336:
3333:
3327:
3324:
3319:
3316:
3313:
3310:
3306:
3302:
3297:
3294:
3291:
3287:
3283:
3280:
3277:
3272:
3269:
3265:
3259:
3255:
3249:
3245:
3239:
3235:
3231:
3225:
3222:
3216:
3211:
3206:
3200:
3197:
3194:
3190:
3186:
3181:
3177:
3172:
3165:
3161:
3155:
3151:
3147:
3141:
3138:
3121:
3120:
3103:
3100:
3096:
3090:
3086:
3080:
3076:
3072:
3069:
3067:
3063:
3056:
3052:
3044:
3040:
3036:
3035:
3030:
3027:
3024:
3021:
3017:
3011:
3008:
3004:
2998:
2994:
2988:
2984:
2980:
2974:
2971:
2967:
2964:
2961:
2957:
2950:
2945:
2942:
2938:
2935:
2931:
2927:
2924:
2921:
2917:
2911:
2907:
2900:
2897:
2892:
2886:
2882:
2875:
2872:
2868:
2864:
2858:
2855:
2850:
2847:
2845:
2841:
2838:
2835:
2831:
2825:
2821:
2815:
2811:
2807:
2806:
2792:
2791:
2776:
2773:
2769:
2762:
2759:
2754:
2750:
2745:
2741:
2736:
2732:
2729:
2727:
2724:
2717:
2714:
2709:
2705:
2700:
2696:
2691:
2687:
2686:
2680:
2677:
2673:
2670:
2666:
2662:
2659:
2656:
2650:
2645:
2642:
2638:
2635:
2631:
2627:
2624:
2621:
2617:
2611:
2607:
2601:
2597:
2594:
2588:
2585:
2583:
2581:
2577:
2571:
2567:
2563:
2558:
2554:
2549:
2543:
2540:
2536:
2533:
2529:
2526:
2522:
2516:
2513:
2510:
2507:
2503:
2497:
2494:
2491:
2487:
2481:
2478:
2473:
2470:
2468:
2465:
2458:
2455:
2450:
2446:
2441:
2437:
2432:
2428:
2427:
2422:
2419:
2416:
2412:
2408:
2405:
2402:
2399:
2397:
2394:
2388:
2384:
2380:
2375:
2371:
2366:
2362:
2361:
2328:
2327:
2312:
2307:
2303:
2297:
2294:
2291:
2288:
2285:
2281:
2275:
2271:
2264:
2260:
2255:
2252:
2250:
2246:
2242:
2238:
2237:
2232:
2228:
2222:
2219:
2216:
2213:
2209:
2203:
2199:
2192:
2188:
2183:
2180:
2178:
2174:
2170:
2166:
2165:
2149:
2142:
2131:
2120:
2078:
2071:
2062:
2061:
2048:
2043:
2037:
2033:
2029:
2024:
2020:
2015:
2008:
2004:
2001:
1997:
1994:
1991:
1988:
1985:
1981:
1975:
1971:
1967:
1962:
1959:
1954:
1948:
1945:
1939:
1934:
1930:
1922:
1917:
1914:
1911:
1907:
1903:
1898:
1867:
1863:
1842:
1822:
1819:
1814:
1810:
1789:
1786:
1781:
1777:
1773:
1768:
1764:
1741:
1737:
1717:
1714:
1697:
1694:
1691:
1688:
1685:
1682:
1679:
1654:
1612:
1593:
1588:
1587:
1576:
1571:
1567:
1564:
1560:
1557:
1554:
1551:
1548:
1543:
1539:
1536:
1528:
1523:
1519:
1514:
1509:
1504:
1500:
1496:
1492:
1486:
1482:
1478:
1473:
1469:
1450:
1449:
1438:
1430:
1426:
1422:
1415:
1411:
1405:
1401:
1394:
1391:
1386:
1382:
1378:
1374:
1371:
1368:
1365:
1361:
1358:
1355:
1352:
1349:
1319:
1316:
1313:
1310:
1307:
1287:
1284:
1281:
1278:
1274:
1270:
1267:
1264:
1261:
1258:
1236:
1233:
1230:
1227:
1223:
1219:
1214:
1210:
1191:
1175:
1174:
1163:
1158:
1155:
1152:
1149:
1145:
1139:
1135:
1129:
1124:
1121:
1118:
1115:
1111:
1107:
1104:
1101:
1097:
1093:
1088:
1084:
1059:
1058:
1047:
1039:
1035:
1031:
1024:
1020:
1014:
1010:
1003:
1000:
996:
990:
987:
984:
980:
976:
971:
968:
965:
961:
956:
952:
949:
944:
940:
936:
933:
930:
894:
872:
871:
870:
869:
868:
867:
866:
865:
864:
863:
862:
861:
860:
859:
858:
857:
851:
841:
830:
825:
796:
795:
794:
793:
792:
791:
790:
789:
788:
787:
786:
785:
784:
783:
782:
781:
724:
721:
706:
703:
649:
646:
629:
616:
615:
604:
599:
594:
588:
584:
580:
575:
571:
566:
559:
555:
551:
545:
542:
534:
530:
527:
523:
520:
517:
514:
511:
507:
492:
491:
436:approximations
411:
406:
405:
393:
387:
383:
379:
374:
370:
365:
361:
356:
353:
350:
346:
340:
337:
296:covalent bonds
261:correspondence
252:
249:
196:
193:
15:
9:
6:
4:
3:
2:
9821:
9810:
9807:
9805:
9802:
9800:
9797:
9796:
9794:
9781:
9780:
9775:
9769:
9763:
9760:
9758:
9755:
9753:
9750:
9748:
9745:
9743:
9740:
9738:
9737:Exotic matter
9735:
9731:
9728:
9727:
9726:
9725:Eightfold way
9723:
9721:
9718:
9716:
9715:Antiparticles
9713:
9711:
9708:
9706:
9703:
9699:
9696:
9695:
9694:
9691:
9687:
9684:
9683:
9682:
9679:
9678:
9676:
9672:
9666:
9663:
9661:
9658:
9656:
9653:
9651:
9648:
9646:
9643:
9642:
9640:
9636:
9630:
9627:
9625:
9622:
9620:
9617:
9615:
9612:
9610:
9607:
9605:
9602:
9600:
9597:
9595:
9592:
9590:
9587:
9585:
9582:
9580:
9577:
9575:
9572:
9570:
9567:
9565:
9562:
9561:
9559:
9557:
9553:
9539:
9536:
9534:
9531:
9529:
9526:
9524:
9521:
9520:
9518:
9514:
9504:
9501:
9499:
9496:
9494:
9491:
9490:
9488:
9484:
9478:
9475:
9473:
9470:
9468:
9465:
9464:
9462:
9458:
9454:
9451:
9449:
9445:
9439:
9436:
9434:
9431:
9427:
9424:
9422:
9419:
9417:
9414:
9412:
9409:
9407:
9404:
9402:
9399:
9398:
9397:
9394:
9392:
9389:
9387:
9386:Atomic nuclei
9384:
9383:
9381:
9377:
9367:
9364:
9361:
9357:
9354:
9353:
9351:
9349:
9345:
9339:
9336:
9334:
9331:
9329:
9326:
9324:
9321:
9319:
9318:Upsilon meson
9316:
9314:
9311:
9309:
9306:
9304:
9301:
9299:
9296:
9294:
9291:
9289:
9286:
9284:
9281:
9280:
9278:
9276:
9272:
9266:
9263:
9261:
9258:
9256:
9253:
9251:
9250:Lambda baryon
9248:
9246:
9243:
9239:
9236:
9234:
9231:
9229:
9226:
9224:
9221:
9220:
9219:
9216:
9215:
9213:
9211:
9207:
9204:
9202:
9198:
9195:
9193:
9189:
9175:
9172:
9170:
9167:
9165:
9162:
9160:
9157:
9155:
9152:
9150:
9147:
9145:
9142:
9140:
9137:
9135:
9132:
9130:
9127:
9125:
9122:
9120:
9117:
9115:
9112:
9110:
9109:Dual graviton
9107:
9105:
9102:
9100:
9097:
9095:
9092:
9091:
9089:
9085:
9074:
9070:
9067:
9065:
9062:
9060:
9057:
9055:
9052:
9050:
9047:
9046:
9044:
9040:
9034:
9031:
9029:
9026:
9024:
9021:
9020:
9018:
9016:
9012:
9009:
9007:
9006:Superpartners
9003:
9000:
8998:
8994:
8988:
8985:
8984:
8982:
8980:
8976:
8966:
8963:
8962:
8960:
8958:
8954:
8948:
8945:
8943:
8940:
8938:
8935:
8934:
8932:
8930:
8926:
8923:
8921:
8917:
8905:
8902:
8900:
8897:
8895:
8892:
8890:
8889:Muon neutrino
8887:
8885:
8882:
8880:
8877:
8876:
8875:
8872:
8870:
8867:
8865:
8862:
8860:
8857:
8855:
8852:
8850:
8847:
8845:
8842:
8841:
8839:
8837:
8833:
8827:
8824:
8822:
8821:Bottom (quark
8819:
8817:
8814:
8812:
8809:
8807:
8804:
8802:
8799:
8797:
8794:
8792:
8789:
8787:
8784:
8782:
8779:
8777:
8774:
8772:
8769:
8768:
8766:
8764:
8760:
8757:
8755:
8751:
8748:
8746:
8742:
8738:
8731:
8726:
8724:
8719:
8717:
8712:
8711:
8708:
8701:
8698:
8695:
8692:
8690:
8687:
8684:
8681:
8678:
8673:
8669:
8668:
8655:
8651:
8647:
8643:
8639:
8635:
8630:
8625:
8621:
8617:
8613:
8606:
8598:
8594:
8590:
8586:
8582:
8578:
8573:
8568:
8565:(1): 011020.
8564:
8560:
8556:
8548:
8540:
8536:
8531:
8526:
8522:
8518:
8514:
8510:
8509:
8504:
8498:
8490:
8484:
8480:
8479:
8471:
8456:
8452:
8446:
8439:
8433:
8426:
8420:
8411:
8406:
8402:
8398:
8394:
8390:
8386:
8382:
8375:
8367:
8363:
8359:
8355:
8351:
8347:
8342:
8337:
8333:
8329:
8322:
8315:
8307:
8301:
8297:
8293:
8292:
8284:
8268:
8264:
8258:
8256:
8247:
8241:
8237:
8230:
8215:
8211:
8205:
8203:
8194:
8188:
8184:
8180:
8179:, 8th Edition
8178:
8170:
8162:
8156:
8152:
8145:
8137:
8135:0-03-083993-9
8131:
8127:
8120:
8118:
8116:
8114:
8112:
8110:
8108:
8099:
8093:
8089:
8085:
8078:
8076:
8067:
8061:
8057:
8053:
8046:
8044:
8035:
8029:
8025:
8018:
8010:
8004:
8000:
7993:
7985:
7983:9780070409545
7979:
7974:
7973:
7964:
7957:
7951:
7949:
7940:
7934:
7930:
7929:
7921:
7913:
7907:
7903:
7896:
7888:
7882:
7874:
7868:
7864:
7863:
7855:
7847:
7841:
7837:
7830:
7828:
7826:
7824:
7822:
7820:
7811:
7805:
7801:
7794:
7790:
7779:
7776:
7774:
7771:
7769:
7766:
7764:
7761:
7759:
7756:
7754:
7751:
7749:
7746:
7744:
7741:
7739:
7738:Rayleigh wave
7736:
7734:
7731:
7729:
7726:
7724:
7721:
7719:
7716:
7714:
7711:
7709:
7706:
7704:
7701:
7699:
7696:
7695:
7690:
7684:
7679:
7672:
7669:
7661:
7659:
7655:
7651:
7647:
7644:vanishes and
7643:
7639:
7630:
7627:
7626:negative mass
7623:
7613:
7611:
7607:
7603:
7593:
7591:
7585:
7581:
7576: =
7573:
7569:
7562:
7545:
7540:
7536:
7530:
7523:
7519:
7511:
7507:
7503:
7500:
7493:
7492:
7491:
7489:
7485:
7481:
7474:
7470:
7441:
7438:
7433:
7430:
7427:
7423:
7419:
7413:
7410:
7405:
7401:
7394:
7389:
7386:
7383:
7379:
7375:
7372:
7367:
7363:
7348:
7344:
7338:
7328:
7323:
7320:
7317:
7313:
7307:
7303:
7297:
7294:
7291:
7287:
7283:
7278:
7274:
7261:
7257:
7249:
7248:
7247:
7223:
7218:
7215:
7212:
7208:
7204:
7198:
7195:
7190:
7186:
7179:
7174:
7171:
7168:
7164:
7160:
7157:
7152:
7148:
7135:
7132:
7127:
7123:
7117:
7107:
7102:
7099:
7096:
7092:
7086:
7082:
7076:
7073:
7070:
7066:
7062:
7057:
7053:
7040:
7033:
7029:
7019:
7018:
7017:
7012:
7006:
6999:
6993:
6990: +
6986:
6980:
6976:
6969:
6965:
6958:
6954:
6942:
6936:
6930:
6924:
6919:
6917:
6913:
6891:
6869:
6868:infinite term
6865:
6843:
6839:
6835:
6813:
6792:
6788:
6782:
6775:
6771:
6763:
6759:
6750:
6746:
6742:
6728:
6727:
6726:
6724:
6704:
6698:
6694:
6687:
6682:
6677:
6673:
6667:
6662:
6658:
6654:
6649:
6644:
6640:
6635:
6629:
6625:
6618:
6615:
6609:
6595:
6594:
6593:
6585:
6583:
6582:heat transfer
6579:
6575:
6571:
6568:behavior (or
6567:
6557:
6555:
6551:
6544:
6539:
6535:
6531:
6509:
6506:
6502:
6495:
6484:
6476:
6473:
6470:
6466:
6462:
6455:
6451:
6448:
6444:
6439:
6435:
6430:
6427:
6424:
6420:
6416:
6412:
6405:
6404:
6403:
6401:
6397:
6393:
6389:
6383:
6381:
6377:
6373:
6369:
6365:
6364:absolute zero
6360:
6357:
6356:heat capacity
6353:
6349:
6348:thermodynamic
6339:
6337:
6336:
6330:
6326:
6317:
6313:
6311:
6303:
6287: ±
6286:
6278:
6262: ±
6261:
6257:
6253:
6232:
6228:
6225:
6222:
6216:
6213:
6206:
6205:
6204:
6185:
6182:
6179:
6154:
6145:
6136:
6131:
6128:
6125:
6121:
6100:
6091:
6087:
6079:
6078:
6077:
6075:
6071:
6067:
6063:
6059:
6055:
6051:
6047:
6044:
6040:
6037:
6033:
6029:
6021:
6016:
6011:
6001:
5999:
5995:
5991:
5987:
5983:
5979:
5974:
5972:
5968:
5964:
5960:
5956:
5951:
5946:
5944:
5940:
5936:
5932:
5928:
5925:
5921:
5919:
5909:
5892:
5888:
5881:
5878:
5872:
5867:
5864:
5861:
5857:
5851:
5844:
5841:
5838:
5834:
5827:
5821:
5818:
5815:
5811:
5801:
5796:
5793:
5790:
5786:
5780:
5776:
5772:
5758:
5757:
5756:
5753:
5751:
5750:
5744:
5740:
5733:
5728:
5726:
5719:
5712:
5704:
5702:
5699:
5695:
5691:
5683:
5677:
5670:
5647:
5640:
5637:
5631:
5626:
5622:
5616:
5609:
5605:
5598:
5592:
5588:
5579:
5575:
5571:
5557:
5556:
5555:
5539:
5512:
5508:
5483:
5477:
5474:
5470:
5466:
5461:
5454:
5450:
5443:
5436:
5430:
5426:
5422:
5419:
5412:
5409:
5404:
5378:
5372:
5369:
5365:
5361:
5356:
5349:
5345:
5338:
5328:
5324:
5320:
5317:
5313:
5307:
5302:
5298:
5290:
5289:
5288:
5286:
5279:
5257:
5254:
5250:
5244:
5236:
5233:
5228:
5222:
5217:
5210:
5206:
5199:
5195:
5182:
5179:
5174:
5170:
5165:
5161:
5149:
5143:
5140:
5136:
5133:
5129:
5125:
5121:
5115:
5107:
5104:
5099:
5093:
5088:
5084:
5079:
5071:
5070:
5069:
5067:
5047:
5041:
5028:
5024:
5020:
5016:
5011:
5006:
5003:
4999:
4994:
4983:
4976:
4972:
4968:
4961:
4956:
4949:
4945:
4921:
4915:
4912:
4899:
4895:
4891:
4887:
4882:
4877:
4873:
4868:
4857:
4850:
4846:
4842:
4835:
4830:
4826:
4818:
4817:
4816:
4814:
4796:
4769:
4765:
4732:
4728:
4724:
4720:
4716:
4712:
4708:
4698:
4696:
4692:
4687:
4682:
4680:
4675:
4671:
4668:
4664:
4660:
4655:
4651:
4649:
4645:
4641:
4637:
4633:
4629:
4625:
4621:
4617:
4609:
4589:
4573:
4569:
4564:
4562:
4558:
4554:
4550:
4542:
4533:
4521:
4516:
4514:
4510:
4506:
4502:
4498:
4495: =
4494:
4489:
4472:
4468:
4465:
4458:
4455:
4447:
4428:
4418:
4414:
4408:
4404:
4396:
4392:
4389:
4383:
4378:
4374:
4370:
4364:
4359:
4354:
4346:
4342:
4338:
4333:
4326:
4322:
4318:
4312:
4305:
4302:
4298:
4290:
4286:
4282:
4277:
4270:
4266:
4262:
4256:
4252:
4249:
4244:
4239:
4235:
4227:
4226:
4225:
4223:
4219:
4212:
4205:
4197:
4193:
4190: =
4189:
4184:
4176:
4168:
4160:
4151:
4149:
4145:
4141:
4137:
4132:
4130:
4126:
4123:
4119:
4108:
4103:
4101:
4096:
4094:
4090:
4086:
4083:
4079:
4074:
4072:
4068:
4064:
4030:
4024:
4015:
4012:
4003:
4000:
3991:
3988:
3979:
3976:
3967:
3964:
3954:
3953:
3952:
3935:
3932:
3929:
3926:
3923:
3920:
3917:
3914:
3911:
3908:
3902:
3898:
3890:
3886:
3883:
3877:
3874:
3867:
3863:
3858:
3854:
3846:
3845:
3844:
3842:
3834:
3832:
3828:
3806:
3801:
3798:
3793:
3790:
3787:
3784:
3781:
3778:
3775:
3772:
3769:
3766:
3763:
3760:
3746:
3743:
3738:
3735:
3732:
3726:
3721:
3717:
3713:
3710:
3703:
3702:
3701:
3699:
3695:
3690:
3688:
3684:
3680:
3676:
3656:
3650:
3647:
3643:
3637:
3633:
3627:
3622:
3618:
3612:
3608:
3604:
3599:
3596:
3586:
3577:
3571:
3567:
3560:
3557:
3553:
3548:
3534:
3533:
3532:
3514:
3508:
3504:
3501:
3495:
3492:
3488:
3484:
3481:
3478:
3472:
3467:
3464:
3460:
3457:
3454:
3451:
3447:
3441:
3437:
3433:
3428:
3423:
3419:
3411:
3410:
3409:
3390:
3387:
3383:
3377:
3373:
3367:
3360:
3356:
3350:
3345:
3341:
3334:
3331:
3325:
3317:
3314:
3311:
3308:
3304:
3300:
3295:
3292:
3289:
3285:
3281:
3278:
3270:
3267:
3263:
3257:
3253:
3247:
3243:
3237:
3233:
3229:
3223:
3220:
3214:
3209:
3204:
3198:
3195:
3192:
3188:
3184:
3179:
3175:
3170:
3163:
3159:
3153:
3149:
3145:
3139:
3136:
3126:
3125:
3124:
3101:
3098:
3088:
3078:
3074:
3070:
3068:
3061:
3054:
3050:
3042:
3038:
3028:
3025:
3022:
3019:
3015:
3009:
3006:
3002:
2996:
2992:
2986:
2982:
2978:
2972:
2969:
2965:
2962:
2959:
2955:
2948:
2943:
2940:
2936:
2933:
2929:
2925:
2922:
2919:
2915:
2909:
2905:
2898:
2895:
2890:
2884:
2880:
2873:
2870:
2866:
2862:
2856:
2853:
2848:
2846:
2839:
2836:
2833:
2829:
2823:
2819:
2813:
2809:
2797:
2796:
2795:
2774:
2771:
2767:
2760:
2757:
2748:
2743:
2734:
2730:
2728:
2722:
2715:
2712:
2707:
2703:
2698:
2694:
2689:
2678:
2675:
2671:
2668:
2664:
2657:
2654:
2648:
2643:
2640:
2636:
2633:
2629:
2625:
2622:
2619:
2615:
2609:
2605:
2599:
2592:
2586:
2584:
2575:
2569:
2565:
2561:
2556:
2552:
2547:
2541:
2538:
2534:
2531:
2527:
2524:
2520:
2514:
2511:
2508:
2505:
2501:
2495:
2492:
2489:
2485:
2479:
2476:
2471:
2469:
2463:
2456:
2453:
2444:
2439:
2435:
2430:
2420:
2417:
2414:
2410:
2403:
2400:
2398:
2392:
2386:
2382:
2378:
2373:
2369:
2364:
2352:
2351:
2350:
2347:
2345:
2337:
2333:
2330:The quantity
2310:
2305:
2301:
2295:
2292:
2289:
2286:
2283:
2279:
2273:
2269:
2262:
2258:
2253:
2251:
2244:
2230:
2226:
2220:
2217:
2214:
2211:
2207:
2201:
2197:
2190:
2186:
2181:
2179:
2172:
2168:
2156:
2155:
2154:
2152:
2145:
2138:
2134:
2127:
2123:
2116:
2111:
2109:
2105:
2101:
2097:
2096:Fourier space
2093:
2089:
2085:
2081:
2074:
2067:
2046:
2041:
2035:
2031:
2027:
2022:
2018:
2013:
1989:
1986:
1979:
1973:
1969:
1965:
1960:
1957:
1952:
1946:
1943:
1937:
1932:
1928:
1920:
1915:
1912:
1909:
1905:
1901:
1887:
1886:
1885:
1883:
1865:
1861:
1840:
1820:
1817:
1812:
1808:
1787:
1784:
1779:
1775:
1771:
1766:
1762:
1739:
1735:
1725:
1723:
1713:
1711:
1695:
1692:
1689:
1683:
1677:
1667:
1663:
1657:
1648:
1635:
1630:
1628:
1624:
1620:
1615:
1606:
1604:
1596:
1574:
1565:
1562:
1558:
1555:
1552:
1549:
1541:
1537:
1534:
1526:
1521:
1517:
1512:
1507:
1502:
1498:
1494:
1490:
1484:
1480:
1476:
1471:
1467:
1459:
1458:
1457:
1455:
1436:
1428:
1424:
1420:
1413:
1409:
1403:
1399:
1392:
1389:
1384:
1380:
1372:
1369:
1366:
1363:
1359:
1356:
1350:
1347:
1340:
1339:
1338:
1336:
1331:
1317:
1314:
1311:
1308:
1305:
1282:
1279:
1272:
1268:
1265:
1262:
1259:
1256:
1234:
1231:
1228:
1225:
1221:
1217:
1212:
1208:
1199:
1194:
1181:
1161:
1156:
1153:
1150:
1147:
1143:
1137:
1133:
1127:
1122:
1119:
1116:
1113:
1109:
1105:
1102:
1099:
1095:
1091:
1086:
1082:
1074:
1073:
1072:
1069:
1067:
1062:
1045:
1037:
1033:
1029:
1022:
1018:
1012:
1008:
1001:
998:
994:
988:
985:
982:
978:
974:
969:
966:
963:
959:
954:
950:
947:
942:
938:
934:
931:
928:
921:
920:
919:
909:
904:
897:
854:
850:
844:
833:
829:
826:
815:
814:
813:
812:
811:
810:
809:
808:
807:
806:
805:
804:
803:
802:
801:
800:
799:
776:
765:
759:
752:
749:
748:
747:
746:
745:
744:
743:
742:
741:
740:
739:
738:
737:
736:
735:
734:
733:
731:
720:
711:
702:
700:
696:
691:
689:
685:
681:
676:
674:
671:
667:
663:
654:
648:Lattice waves
645:
644:
638:
636:
632:
625:
621:
602:
597:
592:
586:
582:
578:
573:
569:
564:
557:
553:
549:
543:
540:
515:
512:
505:
497:
496:
495:
489:
485:
484:
483:
481:
475:
473:
469:
465:
461:
457:
454:
450:
446:
442:
437:
433:
428:
426:
423:th atom, and
422:
418:
414:
391:
385:
381:
377:
372:
368:
363:
359:
354:
351:
348:
344:
338:
335:
326:
325:
324:
321:
317:
313:
312:gravitational
309:
305:
301:
297:
293:
289:
285:
281:
277:
273:
269:
264:
262:
258:
248:
246:
242:
241:particle-like
238:
234:
230:
226:
225:superposition
222:
218:
214:
210:
206:
202:
192:
190:
186:
183:exhibit both
182:
178:
174:
170:
166:
162:
158:
154:
149:
138:
134:
133:Yakov Frenkel
130:
126:
122:
117:
115:
111:
107:
102:
100:
97:as quantized
96:
93:, similar to
92:
88:
84:
81:
77:
76:excited state
73:
69:
68:quasiparticle
65:
61:
57:
53:
49:
45:
41:
37:
30:
26:
22:
9777:
9598:
9448:Hypothetical
9396:Exotic atoms
9265:Omega baryon
9255:Sigma baryon
9245:Delta baryon
8997:Hypothetical
8979:Ghost fields
8965:Higgs boson
8899:Tau neutrino
8791:Charm (quark
8679:at Wikiquote
8619:
8615:
8605:
8562:
8558:
8547:
8512:
8506:
8497:
8477:
8470:
8458:. Retrieved
8454:
8445:
8432:
8419:
8388:
8384:
8374:
8331:
8327:
8314:
8290:
8283:
8271:. Retrieved
8267:News.mit.edu
8266:
8235:
8229:
8217:. Retrieved
8213:
8175:
8169:
8150:
8144:
8125:
8087:
8055:
8023:
8017:
7998:
7992:
7971:
7963:
7955:
7927:
7920:
7901:
7895:
7861:
7854:
7835:
7799:
7793:
7758:Second sound
7670:
7667:
7650:Cooper pairs
7636:
7619:
7599:
7596:Nonlinearity
7583:
7579:
7571:
7567:
7563:
7560:
7476:
7472:
7465:
7463:
7245:
7010:
7004:
6997:
6991:
6984:
6978:
6971:
6970:is given by
6967:
6960:
6956:
6949:
6940:
6934:
6928:
6923:vacuum state
6920:
6908:
6886:
6860:
6830:
6809:
6720:
6591:
6569:
6563:
6553:
6542:
6537:
6533:
6529:
6527:
6384:
6368:ground state
6361:
6345:
6332:
6328:
6324:
6322:
6301:
6284:
6276:
6259:
6255:
6251:
6249:
6202:
6073:
6069:
6061:
6057:
6053:
6049:
6045:
6038:
6032:matter waves
6025:
5981:
5975:
5963:Raman active
5962:
5958:
5947:
5934:
5930:
5929:
5923:
5922:
5915:
5907:
5754:
5746:
5735:
5729:
5721:
5714:
5707:
5705:
5686:
5678:
5672:
5665:
5663:
5499:
5281:
5274:
5272:
5063:
4704:
4695:viscoelastic
4683:
4676:
4672:
4666:
4662:
4658:
4656:
4652:
4643:
4635:
4619:
4607:
4587:
4565:
4560:
4556:
4552:
4540:
4528:
4517:
4512:
4508:
4500:
4496:
4492:
4490:
4445:
4443:
4221:
4217:
4210:
4203:
4201:
4195:
4191:
4187:
4140:polarization
4135:
4133:
4128:
4124:
4117:
4115:
4097:
4084:
4077:
4075:
4062:
4045:
3950:
3837:
3835:
3830:
3826:
3824:
3697:
3693:
3691:
3686:
3678:
3674:
3672:
3530:
3407:
3122:
2793:
2348:
2331:
2329:
2147:
2140:
2136:
2129:
2118:
2114:
2112:
2100:normal modes
2087:
2076:
2069:
2065:
2063:
1833:if particle
1726:
1721:
1719:
1665:
1661:
1652:
1650:held fixed,
1646:
1631:
1621:between the
1610:
1607:
1591:
1589:
1451:
1334:
1332:
1197:
1189:
1179:
1176:
1070:
1063:
1060:
907:
905:
892:
873:
852:
848:
839:
831:
827:
797:
774:
763:
757:
750:
726:
717:
695:normal modes
692:
683:
679:
677:
672:
659:
639:
634:
627:
619:
617:
493:
476:
471:
467:
463:
459:
455:
444:
429:
424:
420:
409:
407:
319:
279:
275:
265:
254:
228:
198:
164:
156:
152:
128:
118:
103:
83:quantization
66:. A type of
35:
33:
9730:Quark model
9498:Theta meson
9401:Positronium
9313:Omega meson
9308:J/psi meson
9238:Antineutron
9149:Dark photon
9114:Graviphoton
9073:Stop squark
8781:Down (quark
7600:As well as
6916:Hamiltonian
6812:Hamiltonian
6378:about some
6372:temperature
4731:eigenvalues
2108:periodicity
2098:which uses
1882:Hamiltonian
1603:normal mode
918:th atom is
878:labels the
699:frequencies
675:is marked.
268:crystalline
221:normal mode
205:vibrational
177:light waves
173:sound waves
127:. The name
99:light waves
91:sound waves
9793:Categories
9472:Heptaquark
9433:Superatoms
9366:Pentaquark
9356:Tetraquark
9338:Quarkonium
9228:Antiproton
9129:Leptoquark
9064:Neutralino
8826:antiquark)
8816:antiquark)
8811:Top (quark
8806:antiquark)
8796:antiquark)
8786:antiquark)
8776:antiquark)
8745:Elementary
8629:2205.05037
8572:2205.05037
8488:0486435032
8395:: 012121.
7785:References
6574:conduction
6388:photon gas
6380:mean value
6036:wavevector
5994:wavelength
5978:wavenumber
4572:wavevector
4122:wavevector
4105:See also:
4080:amount of
2344:wavelength
2336:wavenumber
2104:wavevector
1627:wavenumber
670:wavelength
229:elementary
195:Definition
123:physicist
9710:Particles
9655:Particles
9614:Polariton
9604:Plasmaron
9574:Dropleton
9467:Hexaquark
9438:Molecules
9426:Protonium
9303:Phi meson
9288:Rho meson
9260:Xi baryon
9192:Composite
9028:Gravitino
8771:Up (quark
8654:248665478
8622:(1): 26.
8597:248665478
8539:195774243
8460:13 August
8273:13 August
8219:15 August
7881:cite book
7778:Vibration
7608:and form
7541:α
7531:†
7524:α
7512:α
7508:∑
7442:…
7428:α
7411:−
7406:α
7387:−
7384:α
7373:…
7349:α
7329:…
7318:α
7308:α
7295:−
7292:α
7284:…
7262:α
7224:…
7213:α
7191:α
7172:−
7169:α
7158:…
7128:α
7108:…
7097:α
7087:α
7074:−
7071:α
7063:…
7041:†
7034:α
6946:…⟩
6838:continuum
6793:α
6783:†
6776:α
6764:α
6760:ω
6756:ℏ
6751:α
6747:∑
6699:α
6695:ω
6691:ℏ
6688:−
6678:α
6663:α
6659:ω
6645:α
6630:α
6626:∑
6578:radiation
6507:−
6467:ω
6463:ℏ
6452:
6421:ω
6229:π
6176:Π
6142:Π
5918:unit cell
5852:†
5812:ω
5807:ℏ
5787:∑
5777:∑
5694:hermitian
5617:†
5589:ω
5585:ℏ
5576:∑
5536:Π
5475:−
5467:−
5462:†
5427:ω
5420:ℏ
5401:Π
5370:−
5357:†
5325:ω
5314:ℏ
5245:†
5218:†
5130:δ
5116:†
5038:Π
5025:ω
5012:−
5004:−
4987:ℏ
4973:ω
4957:†
4913:−
4909:Π
4896:ω
4861:ℏ
4847:ω
4793:Π
4693:(but see
4473:λ
4469:π
4384:
4365:−
4303:±
4240:±
4236:ω
4031:⋯
4025:ω
4022:ℏ
4001:ω
3998:ℏ
3977:ω
3974:ℏ
3936:…
3899:ω
3895:ℏ
3794:±
3791:…
3782:±
3773:±
3756:for
3736:π
3683:Hermitian
3648:−
3619:ω
3597:−
3593:Π
3583:Π
3568:∑
3496:
3485:ω
3461:
3455:−
3438:ω
3420:ω
3388:−
3357:ω
3342:∑
3309:−
3301:−
3282:−
3268:−
3244:∑
3234:ω
3185:−
3160:∑
3150:ω
3099:−
3095:Π
3085:Π
3075:∑
3039:∑
3007:−
2983:∑
2906:∑
2863:∑
2810:∑
2753:Π
2740:Π
2665:δ
2661:ℏ
2637:−
2606:∑
2596:ℏ
2525:−
2486:∑
2449:Π
2411:δ
2407:ℏ
2284:−
2270:∑
2241:Π
2198:∑
2113:A set of
2028:−
1980:∑
1970:ω
1906:∑
1788:…
1690:∝
1678:ω
1644:→∞, with
1559:
1553:−
1518:ω
1499:ω
1370:−
1360:
1315:…
1266:π
1209:ϕ
1117:π
1096:∑
986:−
929:−
666:amplitude
579:−
554:ω
506:∑
378:−
352:≠
345:∑
318:function
272:amorphous
237:wave-like
227:of these
213:frequency
191:phonons.
181:unit cell
125:Igor Tamm
62:and some
52:molecules
9686:timeline
9538:R-hadron
9493:Glueball
9477:Skyrmion
9411:Tauonium
9124:Inflaton
9119:Graviton
9099:Curvaton
9069:Sfermion
9059:Higgsino
9054:Chargino
9015:Gauginos
8874:Neutrino
8859:Antimuon
8849:Positron
8844:Electron
8754:Fermions
8455:Phys.org
8366:17019967
7675:See also
7654:exchange
7586:⟩
7574:⟩
7447:⟩
7334:⟩
7229:⟩
7113:⟩
6959:, where
6584:models.
6376:randomly
6043:momentum
5701:spectrum
5237:′
5183:′
5144:′
5108:′
4707:operator
4630:and two
4513:acoustic
3694:periodic
2973:′
2944:′
2899:′
2874:′
2761:′
2716:′
2679:′
2644:′
2535:′
2457:′
2084:momentum
1625:and the
441:screened
417:position
308:Magnetic
304:electric
185:acoustic
9674:Related
9645:Baryons
9619:Polaron
9609:Plasmon
9584:Fracton
9579:Exciton
9533:Diquark
9528:Pomeron
9503:T meson
9460:Baryons
9421:Pionium
9406:Muonium
9333:D meson
9328:B meson
9233:Neutron
9218:Nucleon
9210:Baryons
9201:Hadrons
9164:Tachyon
9139:Majoron
9104:Dilaton
9033:Photino
8869:Antitau
8836:Leptons
8634:Bibcode
8616:Physics
8577:Bibcode
8517:Bibcode
8397:Bibcode
8346:Bibcode
7708:Fracton
7602:photons
6906:
6894:
6884:
6872:
6858:
6846:
6828:
6816:
6548:is the
6306:
6289:
6281:
6264:
6028:photons
5935:optical
4646:in the
4612:
4596:
4592:
4576:
4545:
4524:
4509:optical
4065:is the
4060:
4048:
2128:of the
2102:of the
1632:In the
622:is the
419:of the
415:is the
306:force.
209:lattice
189:optical
95:photons
85:of the
78:in the
72:physics
64:liquids
44:elastic
9804:Bosons
9650:Mesons
9599:Phonon
9594:Magnon
9516:Others
9486:Mesons
9379:Others
9275:Mesons
9223:Proton
9087:Others
9042:Others
9023:Gluino
8957:Scalar
8937:Photon
8920:Bosons
8763:Quarks
8677:Phonon
8652:
8595:
8537:
8508:Nature
8485:
8364:
8302:
8242:
8189:
8157:
8132:
8094:
8062:
8030:
8005:
7980:
7935:
7908:
7869:
7842:
7806:
7622:rotons
7590:bosons
7578:|
7566:|
7475:while
6927:|
6844:, the
6552:, and
6528:where
6333:first
6203:where
5998:photon
5732:bosons
5698:energy
4717:. The
4715:bosons
4686:fluids
4665:and k
4444:where
4089:photon
4082:energy
4046:where
4028:
4007:
3983:
3810:
3408:where
2064:where
1177:Here,
874:where
846:
837:
822:
818:
778:
772:
768:
761:
755:
618:Here,
408:where
288:forces
257:axioms
165:photon
129:phonon
121:Soviet
60:solids
36:phonon
21:photon
9638:Lists
9629:Trion
9624:Roton
9564:Anyon
9391:Atoms
9154:Preon
9094:Axion
9049:Axino
8942:Gluon
8929:Gauge
8650:S2CID
8624:arXiv
8593:S2CID
8567:arXiv
8535:S2CID
8391:(1).
8362:S2CID
8336:arXiv
8324:(PDF)
7753:SASER
7698:Boson
7246:and,
5996:of a
4547:(see
4078:exact
4069:of a
3843:are:
3681:were
2092:waves
1640:→0,
1249:with
714:seen.
662:waves
270:(not
215:. In
161:sound
157:voice
153:sound
148:phonē
139:word
137:Greek
48:atoms
38:is a
27:, or
9589:Hole
9416:Onia
9323:Kaon
9283:Pion
8854:Muon
8696:and
8483:ISBN
8462:2019
8300:ISBN
8275:2019
8240:ISBN
8221:2020
8187:ISBN
8155:ISBN
8130:ISBN
8092:ISBN
8060:ISBN
8028:ISBN
8003:ISBN
7978:ISBN
7933:ISBN
7906:ISBN
7887:link
7867:ISBN
7840:ISBN
7804:ISBN
6346:The
6072:and
6030:and
5713:and
5527:and
5280:and
4640:GaAs
4594:and
3677:and
2135:and
2075:and
1298:for
1071:Put
766:+ 1
753:− 1
310:and
187:and
171:for
142:φωνή
108:and
8864:Tau
8642:doi
8585:doi
8525:doi
8513:571
8405:doi
8389:193
8354:doi
8296:159
8183:100
7490:as
6840:or
6449:exp
6362:At
6056:or
5692:is
4659:ħω.
4375:sin
4076:An
3493:sin
3458:cos
2094:in
1556:cos
1357:cos
906:If
855:+ 1
834:− 1
824:→→→
732:):
482:.)
155:or
101:.
70:in
54:in
50:or
9795::
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8640:.
8632:.
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7879:{{
7818:^
7612:.
7592:.
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6918:.
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6887:ħω
6861:ħω
6831:ħω
6283:,
6050:ħk
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5986:cm
5973:.
5727:.
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5671:=
5068::
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4488:.
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4085:ħω
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4063:ħω
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1659:→
1647:Na
1636:,
1629:.
1605:.
1330:.
1180:na
886:,
816:→→
770:←
701:.
298:,
294:,
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9071:(
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8722:t
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7584:α
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7580:β
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7537:a
7520:a
7504:=
7501:N
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7431:+
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6789:a
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6683:2
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6496:T
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6325:k
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6294:π
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6273:/
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6260:k
6256:k
6252:n
6233:a
6226:n
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6217:=
6214:K
6186:K
6183:+
6180:k
6167:f
6164:e
6161:d
6155:=
6146:k
6137:;
6132:K
6129:+
6126:k
6122:Q
6113:f
6110:e
6107:d
6101:=
6092:k
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6074:Π
6070:Q
6062:k
6039:k
5982:ω
5893:.
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5882:2
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5868:s
5865:,
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5845:s
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5835:b
5828:(
5822:s
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5816:k
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5797:1
5794:=
5791:s
5781:k
5773:=
5768:H
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5736:b
5724:k
5717:k
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5710:k
5708:b
5689:k
5687:n
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5675:k
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5641:2
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5632:+
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5623:b
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5599:(
5593:k
5580:k
5572:=
5567:H
5540:k
5513:k
5509:Q
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5478:k
5471:b
5455:k
5451:b
5444:(
5437:2
5431:k
5423:m
5413:i
5410:=
5405:k
5379:)
5373:k
5366:b
5362:+
5350:k
5346:b
5339:(
5329:k
5321:m
5318:2
5308:=
5303:k
5299:Q
5284:k
5282:b
5277:k
5275:b
5258:0
5255:=
5251:]
5234:k
5229:b
5223:,
5211:k
5207:b
5200:[
5196:=
5191:]
5180:k
5175:b
5171:,
5166:k
5162:b
5156:[
5150:,
5141:k
5137:,
5134:k
5126:=
5122:]
5105:k
5100:b
5094:,
5089:k
5085:b
5080:[
5048:)
5042:k
5029:k
5021:m
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5007:k
5000:Q
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4984:2
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4969:m
4962:=
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4922:)
4916:k
4900:k
4892:m
4888:i
4883:+
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4869:(
4858:2
4851:k
4843:m
4836:=
4831:k
4827:b
4797:k
4770:k
4766:Q
4743:H
4667:.
4663:ω
4644:k
4636:N
4620:N
4608:a
4604:/
4600:π
4588:a
4584:/
4580:π
4561:k
4553:k
4541:k
4539:∂
4536:/
4531:k
4529:ω
4527:∂
4501:k
4499:(
4497:ω
4493:ω
4466:2
4459:=
4456:k
4446:k
4429:,
4419:2
4415:m
4409:1
4405:m
4397:2
4393:a
4390:k
4379:2
4371:4
4360:2
4355:)
4347:2
4343:m
4339:1
4334:+
4327:1
4323:m
4319:1
4313:(
4306:K
4299:)
4291:2
4287:m
4283:1
4278:+
4271:1
4267:m
4263:1
4257:(
4253:K
4250:=
4245:2
4222:K
4218:a
4214:2
4211:m
4207:1
4204:m
4196:k
4194:(
4192:ω
4188:ω
4136:s
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4125:k
4118:k
4057:2
4054:/
4051:1
4016:2
4013:5
4004:,
3992:2
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3980:,
3968:2
3965:1
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3930:,
3927:2
3924:,
3921:1
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3915:0
3912:=
3909:n
3903:k
3891:)
3887:n
3884:+
3878:2
3875:1
3868:(
3864:=
3859:n
3855:E
3840:k
3838:ω
3831:a
3827:n
3807:.
3802:2
3799:N
3788:,
3785:2
3779:,
3776:1
3770:,
3767:0
3764:=
3761:n
3747:a
3744:N
3739:n
3733:2
3727:=
3722:n
3718:k
3714:=
3711:k
3698:N
3687:N
3679:Π
3675:Q
3657:)
3651:k
3644:Q
3638:k
3634:Q
3628:2
3623:k
3613:2
3609:m
3605:+
3600:k
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3578:(
3572:k
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3558:2
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3549:=
3544:H
3515:|
3509:2
3505:a
3502:k
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3482:2
3479:=
3473:)
3468:a
3465:k
3452:1
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3442:2
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3429:=
3424:k
3391:k
3384:Q
3378:k
3374:Q
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3361:k
3351:m
3346:k
3335:2
3332:1
3326:=
3323:)
3318:a
3315:k
3312:i
3305:e
3296:a
3293:k
3290:i
3286:e
3279:2
3276:(
3271:k
3264:Q
3258:k
3254:Q
3248:k
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3230:m
3224:2
3221:1
3215:=
3210:2
3205:)
3199:1
3196:+
3193:j
3189:x
3180:j
3176:x
3171:(
3164:j
3154:2
3146:m
3140:2
3137:1
3102:k
3089:k
3079:k
3071:=
3062:2
3055:l
3051:p
3043:l
3029:k
3026:m
3023:a
3020:i
3016:e
3010:k
3003:Q
2997:k
2993:Q
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2979:=
2970:k
2966:m
2963:a
2960:i
2956:e
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2941:k
2937:+
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2930:(
2926:l
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2916:e
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2871:k
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2857:N
2854:1
2849:=
2840:m
2837:+
2834:l
2830:x
2824:l
2820:x
2814:l
2775:0
2772:=
2768:]
2758:k
2749:,
2744:k
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2731:=
2723:]
2713:k
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2676:k
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2587:=
2576:]
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2542:m
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2472:=
2464:]
2454:k
2445:,
2440:k
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2431:[
2421:m
2418:,
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2401:=
2393:]
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2379:,
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2370:x
2365:[
2340:π
2332:k
2311:.
2306:l
2302:p
2296:l
2293:a
2290:k
2287:i
2280:e
2274:l
2263:N
2259:1
2254:=
2245:k
2231:l
2227:x
2221:l
2218:a
2215:k
2212:i
2208:e
2202:l
2191:N
2187:1
2182:=
2173:k
2169:Q
2150:k
2148:p
2143:k
2141:Π
2137:N
2132:k
2130:x
2121:k
2119:Q
2115:N
2088:i
2079:i
2077:p
2072:i
2070:x
2066:m
2047:2
2042:)
2036:j
2032:x
2023:i
2019:x
2014:(
2007:)
2003:n
2000:n
1996:(
1993:}
1990:j
1987:i
1984:{
1974:2
1966:m
1961:2
1958:1
1953:+
1947:m
1944:2
1938:2
1933:i
1929:p
1921:N
1916:1
1913:=
1910:i
1902:=
1897:H
1866:i
1862:x
1841:i
1821:0
1818:=
1813:i
1809:x
1785:,
1780:2
1776:x
1772:,
1767:1
1763:x
1740:i
1736:u
1722:N
1696:a
1693:k
1687:)
1684:k
1681:(
1668:)
1666:x
1664:(
1662:φ
1655:n
1653:u
1642:N
1638:a
1613:k
1611:ω
1599:k
1594:k
1592:Q
1575:.
1570:)
1566:a
1563:k
1550:1
1547:(
1542:m
1538:C
1535:2
1527:=
1522:k
1513:;
1508:t
1503:k
1495:i
1491:e
1485:k
1481:A
1477:=
1472:k
1468:Q
1437:.
1429:2
1425:t
1421:d
1414:k
1410:Q
1404:2
1400:d
1393:m
1390:=
1385:k
1381:Q
1377:)
1373:1
1367:a
1364:k
1354:(
1351:C
1348:2
1318:N
1312:1
1309:=
1306:j
1286:)
1283:a
1280:N
1277:(
1273:/
1269:j
1263:2
1260:=
1257:k
1235:a
1232:n
1229:k
1226:i
1222:e
1218:=
1213:k
1192:k
1190:Q
1185:x
1162:.
1157:a
1154:n
1151:k
1148:i
1144:e
1138:k
1134:Q
1128:N
1123:1
1120:=
1114:2
1110:/
1106:k
1103:a
1100:N
1092:=
1087:n
1083:u
1046:.
1038:2
1034:t
1030:d
1023:n
1019:u
1013:2
1009:d
1002:m
999:=
995:)
989:1
983:n
979:u
975:+
970:1
967:+
964:n
960:u
955:(
951:C
948:+
943:n
939:u
935:C
932:2
916:n
912:m
908:C
901:n
895:n
893:u
888:a
884:N
880:n
876:n
853:n
849:u
842:n
840:u
832:n
828:u
820:→
780:→
775:a
764:n
758:n
751:n
728:(
684:a
680:a
673:λ
635:i
630:i
628:R
620:ω
603:.
598:2
593:)
587:j
583:R
574:i
570:R
565:(
558:2
550:m
544:2
541:1
533:)
529:n
526:n
522:(
519:}
516:j
513:i
510:{
472:x
468:x
464:x
460:V
456:V
445:V
425:V
421:i
412:i
410:r
392:)
386:j
382:r
373:i
369:r
364:(
360:V
355:j
349:i
339:2
336:1
320:V
280:N
276:N
145:(
31:.
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