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Bubble chamber

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Bubbles grow in size as the chamber expands, until they are large enough to be seen or photographed. Several cameras are mounted around it, allowing a three-dimensional image of an event to be captured. Bubble chambers with resolutions down to a few
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The need for a photographic readout rather than three-dimensional electronic data makes it less convenient, especially in experiments which must be reset, repeated and analyzed many times.
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The high-energy particles may have path radii too large to be accurately measured in a relatively small chamber, thereby hindering precise estimation of momentum.
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Although bubble chambers were very successful in the past, they are of limited use in modern very-high-energy experiments for a variety of reasons:
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Bubble chambers are neither large nor massive enough to analyze high-energy collisions, where all products should be contained inside the detector.
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and their velocities. Because the magnitude of the charge of all known, charged, long-lived subatomic particles is the same as that of an
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The superheated phase must be ready at the precise moment of collision, which complicates the detection of short-lived particles.
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It is often useful to subject the entire chamber to a constant magnetic field. It acts on charged particles through
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phase. Charged particles create an ionization track, around which the liquid vaporizes, forming microscopic
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Donald A. Glaser (1952). "Some Effects of Ionizing Radiation on the Formation of Bubbles in Liquids".
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While bubble chambers were extensively used in the past, they have now mostly been supplanted by
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suddenly decreases its pressure, and the liquid enters into a superheated,
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to be measured at the same time. Another alternative technique is the
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Notable discoveries made by bubble chamber include the discovery of
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Due to these issues, bubble chambers have largely been replaced by
167: 163: 23: 533: 513: 240: 562:"A step-by-step tutorial on how to read bubble chamber pictures" 277: 128: 76:. Supposedly, Glaser was inspired by the bubbles in a glass of 57: 316:, a particle accelerator with a liquid hydrogen bubble chamber 489: 485: 236: 155: 565: 460: 340: 231:). Recently, bubble chambers have been used in research on 183: 77: 166:, their radius of curvature must be proportional to their 68:
particles moving through it. It was invented in 1952 by
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Vessel filled with a superheated transparent liquid
578: 360: 215:in 1973, which established the soundness of the 26:'s disused 15-foot (4.57 m) bubble chamber 421: 233:weakly interacting massive particles (WIMP)s 29: 18: 579: 202: 103:. Notable bubble chambers include the 457:"1973: Neutral currents are revealed" 432:Lawrence Berkeley National Laboratory 127:. As particles enter the chamber, a 72:, for which he was awarded the 1960 119:The bubble chamber is similar to a 114: 13: 309:Berne Infinitesimal Bubble Chamber 14: 603: 554: 399:"The Nobel Prize in Physics 1960" 325:Holographic Lexan Bubble Chamber 219:and led to the discovery of the 190: 182:A bubble chamber recording from 175: 526: 502: 478: 449: 422:Anne Pinckard (21 July 2006). 415: 391: 354: 1: 347: 154:and causes them to travel in 34:The first tracks observed in 250: 7: 320:Big European Bubble Chamber 299:81 cm Saclay Bubble Chamber 294:30 cm Bubble Chamber (CERN) 287: 105:Big European Bubble Chamber 10: 608: 50:is a vessel filled with a 38:'s 1.5-inch (3.8 cm) 486:"COUPP experiment – E961" 428:Berkeley Lab View Archive 304:2 m Bubble Chamber (CERN) 510:"The PICASSO experiment" 42:bubble chamber, in 1954. 276:, which allow particle 385:10.1103/PhysRev.87.665 74:Nobel Prize in Physics 43: 27: 587:Hydrogen technologies 534:"The PICO experiment" 209:weak neutral currents 160:charge-to-mass ratios 33: 22: 403:The Nobel Foundation 336:LExan Bubble Chamber 147:have been operated. 66:electrically charged 377:1952PhRv...87..665G 243:and more recently, 203:Notable discoveries 592:Particle detectors 217:electroweak theory 44: 28: 101:silicon detectors 64:) used to detect 599: 573: 572:on 7 March 2012. 568:. Archived from 548: 547: 545: 544: 530: 524: 523: 521: 520: 506: 500: 499: 497: 496: 482: 476: 475: 473: 472: 463:. Archived from 453: 447: 446: 444: 443: 434:. Archived from 419: 413: 412: 410: 409: 395: 389: 388: 358: 223:in 1983 (at the 197:A bubble chamber 194: 179: 145:micrometers (μm) 115:Function and use 70:Donald A. Glaser 607: 606: 602: 601: 600: 598: 597: 596: 577: 576: 560: 557: 552: 551: 542: 540: 532: 531: 527: 518: 516: 508: 507: 503: 494: 492: 484: 483: 479: 470: 468: 455: 454: 450: 441: 439: 420: 416: 407: 405: 397: 396: 392: 364:Physical Review 359: 355: 350: 290: 253: 229:UA2 experiments 205: 198: 195: 186: 180: 117: 62:liquid hydrogen 40:liquid hydrogen 17: 12: 11: 5: 605: 595: 594: 589: 575: 574: 556: 555:External links 553: 550: 549: 525: 501: 477: 448: 414: 390: 352: 351: 349: 346: 345: 344: 338: 333: 327: 322: 317: 311: 306: 301: 296: 289: 286: 270: 269: 266: 263: 260: 252: 249: 221:W and Z bosons 204: 201: 200: 199: 196: 189: 187: 181: 174: 116: 113: 97:drift chambers 93:spark chambers 48:bubble chamber 15: 9: 6: 4: 3: 2: 604: 593: 590: 588: 585: 584: 582: 571: 567: 563: 559: 558: 539: 535: 529: 515: 511: 505: 491: 487: 481: 467:on 2010-11-16 466: 462: 458: 452: 438:on 2017-12-24 437: 433: 429: 425: 418: 404: 400: 394: 386: 382: 378: 374: 370: 366: 365: 357: 353: 342: 339: 337: 334: 331: 328: 326: 323: 321: 318: 315: 312: 310: 307: 305: 302: 300: 297: 295: 292: 291: 285: 283: 282:spark chamber 279: 275: 274:wire chambers 267: 264: 261: 258: 257: 256: 248: 246: 242: 238: 235:, at SIMPLE, 234: 230: 226: 222: 218: 214: 210: 193: 188: 185: 178: 173: 172: 171: 169: 165: 161: 157: 153: 152:Lorentz force 148: 146: 140: 138: 134: 130: 126: 125:boiling point 122: 121:cloud chamber 112: 110: 106: 102: 98: 94: 90: 89:wire chambers 85: 83: 79: 75: 71: 67: 63: 59: 56: 53: 49: 41: 37: 32: 25: 21: 570:the original 541:. Retrieved 528: 517:. Retrieved 504: 493:. Retrieved 480: 469:. Retrieved 465:the original 451: 440:. Retrieved 436:the original 427: 417: 406:. Retrieved 393: 368: 362: 356: 271: 254: 206: 149: 141: 118: 86: 60:(most often 47: 45: 107:(BEBC) and 55:transparent 52:superheated 581:Categories 543:2016-02-22 519:2009-10-03 495:2009-10-03 471:2009-10-03 442:2009-10-03 408:2009-10-03 371:(4): 665. 348:References 330:Gargamelle 213:Gargamelle 133:metastable 109:Gargamelle 82:prototypes 251:Drawbacks 36:John Wood 314:Bevatron 288:Examples 278:energies 168:momentum 164:electron 24:Fermilab 514:PICASSO 373:Bibcode 241:PICASSO 156:helical 137:bubbles 129:piston 99:, and 58:liquid 490:COUPP 237:COUPP 566:CERN 538:PICO 461:CERN 341:PICO 245:PICO 227:and 184:CERN 78:beer 381:doi 225:UA1 211:at 583:: 564:. 536:. 512:. 488:. 459:. 430:. 426:. 401:. 379:. 369:87 367:. 284:. 247:. 239:, 111:. 95:, 91:, 84:. 46:A 546:. 522:. 498:. 474:. 445:. 411:. 387:. 383:: 375::

Index


Fermilab

John Wood
liquid hydrogen
superheated
transparent
liquid
liquid hydrogen
electrically charged
Donald A. Glaser
Nobel Prize in Physics
beer
prototypes
wire chambers
spark chambers
drift chambers
silicon detectors
Big European Bubble Chamber
Gargamelle
cloud chamber
boiling point
piston
metastable
bubbles
micrometers (μm)
Lorentz force
helical
charge-to-mass ratios
electron

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