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2279: 1980: 385: 2849: 1990: 1691: 1112: 706: 1256: 944: 1376: 2428: 2594:) theorem provides sufficient conditions for a singular integral operator to be a Calderón–Zygmund operator, that is for a singular integral operator associated to a Calderón–Zygmund kernel to be bounded on 1452: 799: 1533: 2554: 1681: 488: 251: 3155:
David; Semmes; Journé (1985). "Opérateurs de Calderón–Zygmund, fonctions para-accrétives et interpolation" (in French). Vol. 1. Revista Matemática Iberoamericana. pp. 1–56.
2711: 2274:{\displaystyle |K(x,y)-K(x,y')|\leq {\frac {C|y-y'|^{\delta }}{{\bigl (}|x-y|+|x-y'|{\bigr )}^{n+\delta }}}{\text{ whenever }}|y-y'|\leq {\frac {1}{2}}\max {\bigl (}|x-y'|,|x-y|{\bigr )}} 1975:{\displaystyle |K(x,y)-K(x',y)|\leq {\frac {C|x-x'|^{\delta }}{{\bigl (}|x-y|+|x'-y|{\bigr )}^{n+\delta }}}{\text{ whenever }}|x-x'|\leq {\frac {1}{2}}\max {\bigl (}|x-y|,|x'-y|{\bigr )}} 127: 989: 2991: 3081: 3029: 196:| > ε as ε → 0, but in practice this is a technicality. Usually further assumptions are required to obtain results such as their boundedness on 526: 582: 1125:. Neither of the properties 1. or 2. is necessarily easy to verify, and a variety of sufficient conditions exist. Typically in applications, one also has a 188:| → 0. Since such integrals may not in general be absolutely integrable, a rigorous definition must define them as the limit of the integral over | 3485: 1135: 1546:
These are even more general operators. However, since our assumptions are so weak, it is not necessarily the case that these operators are bounded on
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Observe that these conditions are satisfied for the Hilbert and Riesz transforms, so this result is an extension of those result.
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The smoothness condition 2. is also often difficult to check in principle, the following sufficient condition of a kernel
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and are intimately connected with the study of partial differential equations. Broadly speaking a singular integral is an
1603: 412: 380:{\displaystyle H(f)(x)={\frac {1}{\pi }}\lim _{\varepsilon \to 0}\int _{|x-y|>\varepsilon }{\frac {1}{x-y}}f(y)\,dy.} 2844:{\displaystyle \left|\int T{\bigl (}\tau ^{x}(\varphi _{r}){\bigr )}(y)\tau ^{x}(\psi _{r})(y)\,dy\right|\leq Cr^{-n}} 3503: 3474: 3447: 3303: 48: 3234: 1107:{\displaystyle \operatorname {p.v.} \,\,K=\lim _{\epsilon \to 0^{+}}\int _{|x|>\epsilon }\phi (x)K(x)\,dx} 3566: 2942: 567: 3298:, Cambridge Studies in Advanced Mathematics, vol. 48, Cambridge University Press, pp. xx+315, 3571: 3495: 3084: 3040: 3032: 149: 3576: 981: 2998: 3491: 701:{\displaystyle T(f)(x)=\lim _{\varepsilon \to 0}\int _{|y-x|>\varepsilon }K(x-y)f(y)\,dy.} 3513: 3457: 3401: 3349: 3313: 3271: 3209: 2922:
if it satisfies all of the following three conditions for some bounded accretive functions
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are smooth and have disjoint support. Such operators need not be bounded on
1266: 3333: 939:{\displaystyle \sup _{y\neq 0}\int _{|x|>2|y|}|K(x-y)-K(x)|\,dx\leq C.} 3481: 28: 3431: 3291: 3263: 3192: 2562:
It can be proved that such operators are, in fact, also bounded on all
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Stein, Elias (1993). "Harmonic Analysis". Princeton University Press.
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supported in a ball of radius 1 and centred at the origin such that |
1371:{\displaystyle \sup _{R>0}\int _{R<|x|<2R}|K(x)|\,dx\leq C,} 390:
The most straightforward higher dimension analogues of these are the
3247: 1269:. If, in addition, one assumes 2. and the following size condition 2423:{\displaystyle \int g(x)T(f)(x)\,dx=\iint g(x)K(x,y)f(y)\,dy\,dx,} 1261:
which is quite easy to check. It is automatic, for instance, if
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Singular integrals and differentiability properties of functions
2598:. In order to state the result we must first define some terms. 3427: 3373: 3369: 2286: 3385: 1541: 1587:
if it satisfies the following conditions for some constants
1447:{\displaystyle K\in C^{1}(\mathbf {R} ^{n}\setminus \{0\})} 794:{\displaystyle {\hat {K}}\in L^{\infty }(\mathbf {R} ^{n})} 3366:
Multidimensional singular integrals and integral equations
3176:(1952), "On the existence of certain singular integrals", 547: 1528:{\displaystyle |\nabla K(x)|\leq {\frac {C}{|x|^{n+1}}}} 3537:"Singular Integrals: The Roles of Calderón and Zygmund" 558:
A singular integral of convolution type is an operator
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associated to a Calderón–Zygmund kernel is bounded on
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Wavelets: Calderón-Zygmund and multilinear operators
2549:{\displaystyle \|T(f)\|_{L^{2}}\leq C\|f\|_{L^{2}},} 2914:) theorem states that a singular integral operator 2899:the operator given by multiplication by a function 1676:{\displaystyle |K(x,y)|\leq {\frac {C}{|x-y|^{n}}}} 483:{\displaystyle K_{i}(x)={\frac {x_{i}}{|x|^{n+1}}}} 3242:(2), The Johns Hopkins University Press: 289–309, 3075: 3023: 2985: 2843: 2548: 2422: 2296:singular integral operator of non-convolution type 2273: 1974: 1675: 1527: 1446: 1370: 1250: 1106: 966:Property 1. is needed to ensure that convolution ( 963:) and satisfies a weak-type (1, 1) estimate. 938: 793: 700: 520: 482: 379: 121: 3154: 218:The archetypal singular integral operator is the 3558: 3416: 2298:associated to the Calderón–Zygmund kernel 2208: 1909: 1280: 1025: 823: 611: 290: 225:. It is given by convolution against the kernel 3490:, Princeton Mathematical Series, vol. 30, 3224: 3168: 554:Singular integral operators of convolution type 160:. Specifically, the singularity is such that | 2456:associated to a Calderón–Zygmund kernel 2761: 2728: 2697: > 0. An operator is said to be 2447: 2266: 2213: 2146: 2092: 1967: 1914: 1847: 1793: 544:and satisfy weak-type (1, 1) estimates. 3545:Notices of the American Mathematical Society 3286: 3106:Singular integral operators on closed curves 2527: 2520: 2498: 2482: 2452:A singular integral of non-convolution type 1438: 1432: 122:{\displaystyle T(f)(x)=\int K(x,y)f(y)\,dy,} 1553: 3135: 3133: 3131: 2287:Singular integrals of non-convolution type 1542:Singular integrals of non-convolution type 3191: 2810: 2625:)| ≤ 1, for all multi-indices | 2410: 2403: 2348: 1352: 1197: 1097: 1008: 1007: 920: 688: 367: 109: 3139: 540:. All of these operators are bounded on 207: 3360: 3328: 3128: 14: 3559: 2559:for all smooth compactly supported ƒ. 1381:then it can be shown that 1. follows. 548:Singular integrals of convolution type 3534: 3480: 3144:, New Jersey: Pearson Education, Inc. 3142:Classical and Modern Fourier Analysis 3123: 562:defined by convolution with a kernel 3117: 576: 2986:{\displaystyle M_{b_{2}}TM_{b_{1}}} 2573: 724:Suppose that the kernel satisfies: 24: 3091:is the transpose operator of  1467: 1216: 1000: 994: 768: 25: 3588: 3528: 3232:(1956), "On singular integrals", 1429: 3535:Stein, Elias M. (October 1998). 2448:Calderón–Zygmund operators 1419: 778: 3420:; Prössdorf, Siegfried (1986), 3235:American Journal of Mathematics 2870: > 0 such that Re( 2462:Calderón–Zygmund operator 3148: 3140:Grafakos, Loukas (2004), "7", 3067: 3054: 3018: 3005: 2807: 2801: 2798: 2785: 2772: 2766: 2756: 2743: 2494: 2488: 2400: 2394: 2388: 2376: 2370: 2364: 2345: 2339: 2336: 2330: 2324: 2318: 2260: 2246: 2238: 2219: 2191: 2172: 2139: 2120: 2112: 2098: 2078: 2058: 2044: 2040: 2023: 2014: 2002: 1995: 1961: 1942: 1934: 1920: 1892: 1873: 1840: 1821: 1813: 1799: 1779: 1759: 1745: 1741: 1724: 1715: 1703: 1696: 1660: 1645: 1631: 1627: 1615: 1608: 1506: 1497: 1483: 1479: 1473: 1463: 1441: 1414: 1348: 1344: 1338: 1331: 1315: 1307: 1194: 1188: 1166: 1158: 1094: 1088: 1082: 1076: 1061: 1053: 1032: 1018: 1012: 916: 912: 906: 897: 885: 878: 871: 863: 852: 844: 788: 773: 754: 685: 679: 673: 661: 646: 632: 618: 604: 598: 595: 589: 461: 452: 432: 426: 364: 358: 325: 311: 297: 273: 267: 264: 258: 106: 100: 94: 82: 70: 64: 61: 55: 13: 1: 3334:"Singular integral equations" 3162: 3076:{\displaystyle T^{t}(b_{2}),} 2472: > 0 such that 7: 3423:Singular Integral Operators 3099: 2862:. A function is said to be 968: 714: 10: 3593: 3496:Princeton University Press 2633: + 2. Denote by 951:Then it can be shown that 551: 211: 2854:for all normalised bumps 3111: 3024:{\displaystyle T(b_{1})} 1554:Calderón–Zygmund kernels 982:principal value integral 574:\{0}, in the sense that 2866:if there is a constant 2701:if there is a constant 18:Calderón–Zygmund kernel 3077: 3025: 2987: 2938: 2845: 2566:with 1 <  2550: 2468:, that is, there is a 2464:when it is bounded on 2424: 2275: 1976: 1677: 1597: 1591: > 0 and 1529: 1448: 1372: 1252: 1108: 940: 795: 702: 522: 484: 381: 132:whose kernel function 123: 3469:, (European edition: 3078: 3026: 2988: 2846: 2605:is a smooth function 2551: 2425: 2276: 1977: 1678: 1530: 1449: 1373: 1253: 1109: 974:tempered distribution 941: 796: 703: 523: 521:{\displaystyle x_{i}} 485: 382: 208:The Hilbert transform 180:| asymptotically as | 124: 3498:, pp. XIV+287, 3396:, pp. XII+255, 3041: 2999: 2943: 2712: 2479: 2309: 2168: whenever  1991: 1869: whenever  1692: 1604: 1459: 1395: 1276: 1136: 990: 819: 809:condition: for some 745: 583: 505: 413: 252: 49: 3418:Mikhlin, Solomon G. 3362:Mikhlin, Solomon G. 3330:Mikhlin, Solomon G. 2570: < ∞. 1595: > 0. 813: > 0, 192: −  184: −  176: −  152:along the diagonal 3567:Singular integrals 3193:10.1007/BF02392130 3073: 3021: 2993:is weakly bounded; 2983: 2841: 2546: 2420: 2271: 1972: 1673: 1525: 1444: 1368: 1294: 1248: 1119:Fourier multiplier 1117:is a well-defined 1104: 1046: 936: 837: 791: 698: 625: 568:locally integrable 518: 480: 377: 304: 245:. More precisely, 233:) = 1/(π 119: 33:singular integrals 3572:Harmonic analysis 2206: 2169: 2164: 1907: 1870: 1865: 1671: 1523: 1279: 1215: 1024: 822: 757: 734:Fourier transform 732:condition on the 722: 721: 610: 532:-th component of 478: 353: 289: 287: 220:Hilbert transform 214:Hilbert transform 41:integral operator 37:harmonic analysis 16:(Redirected from 3584: 3553: 3541: 3524: 3468: 3412: 3352: 3324: 3282: 3220: 3195: 3179:Acta Mathematica 3157: 3156: 3152: 3146: 3145: 3137: 3126: 3125: 3121: 3082: 3080: 3079: 3074: 3066: 3065: 3053: 3052: 3030: 3028: 3027: 3022: 3017: 3016: 2992: 2990: 2989: 2984: 2982: 2981: 2980: 2979: 2962: 2961: 2960: 2959: 2850: 2848: 2847: 2842: 2840: 2839: 2821: 2817: 2797: 2796: 2784: 2783: 2765: 2764: 2755: 2754: 2742: 2741: 2732: 2731: 2555: 2553: 2552: 2547: 2542: 2541: 2540: 2539: 2513: 2512: 2511: 2510: 2429: 2427: 2426: 2421: 2294:is said to be a 2280: 2278: 2277: 2272: 2270: 2269: 2263: 2249: 2241: 2236: 2222: 2217: 2216: 2207: 2199: 2194: 2189: 2175: 2170: 2167: 2165: 2163: 2162: 2161: 2150: 2149: 2142: 2137: 2123: 2115: 2101: 2096: 2095: 2088: 2087: 2086: 2081: 2075: 2061: 2052: 2047: 2039: 1998: 1981: 1979: 1978: 1973: 1971: 1970: 1964: 1953: 1945: 1937: 1923: 1918: 1917: 1908: 1900: 1895: 1890: 1876: 1871: 1868: 1866: 1864: 1863: 1862: 1851: 1850: 1843: 1832: 1824: 1816: 1802: 1797: 1796: 1789: 1788: 1787: 1782: 1776: 1762: 1753: 1748: 1734: 1699: 1682: 1680: 1679: 1674: 1672: 1670: 1669: 1668: 1663: 1648: 1639: 1634: 1611: 1576:is said to be a 1575: 1534: 1532: 1531: 1526: 1524: 1522: 1521: 1520: 1509: 1500: 1491: 1486: 1466: 1453: 1451: 1450: 1445: 1428: 1427: 1422: 1413: 1412: 1377: 1375: 1374: 1369: 1351: 1334: 1329: 1328: 1318: 1310: 1293: 1257: 1255: 1254: 1249: 1241: 1240: 1228: 1227: 1213: 1184: 1183: 1182: 1181: 1169: 1161: 1153: 1152: 1113: 1111: 1110: 1105: 1072: 1071: 1064: 1056: 1045: 1044: 1043: 1006: 945: 943: 942: 937: 919: 881: 876: 875: 874: 866: 855: 847: 836: 800: 798: 797: 792: 787: 786: 781: 772: 771: 759: 758: 750: 716: 707: 705: 704: 699: 657: 656: 649: 635: 624: 577: 527: 525: 524: 519: 517: 516: 489: 487: 486: 481: 479: 477: 476: 475: 464: 455: 449: 448: 439: 425: 424: 402:) = 1/ 394:, which replace 392:Riesz transforms 386: 384: 383: 378: 354: 352: 338: 336: 335: 328: 314: 303: 288: 280: 128: 126: 125: 120: 21: 3592: 3591: 3587: 3586: 3585: 3583: 3582: 3581: 3557: 3556: 3552:(9): 1130–1140. 3539: 3531: 3506: 3450: 3442:, p. 528, 3440:Springer Verlag 3306: 3288:Coifman, Ronald 3248:10.2307/2372517 3226:Calderon, A. P. 3170:Calderon, A. 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1337: 1333: 1327: 1324: 1321: 1317: 1313: 1309: 1305: 1302: 1298: 1292: 1289: 1286: 1282: 1259: 1258: 1247: 1244: 1239: 1235: 1231: 1226: 1222: 1218: 1212: 1209: 1206: 1203: 1200: 1196: 1193: 1190: 1187: 1180: 1176: 1172: 1168: 1164: 1160: 1156: 1151: 1147: 1142: 1115: 1114: 1103: 1100: 1096: 1093: 1090: 1087: 1084: 1081: 1078: 1075: 1070: 1067: 1063: 1059: 1055: 1050: 1042: 1038: 1034: 1031: 1027: 1023: 1020: 1017: 1014: 1011: 1005: 1002: 999: 996: 955:is bounded on 949: 948: 947: 946: 935: 932: 929: 926: 923: 918: 914: 911: 908: 905: 902: 899: 896: 893: 890: 887: 884: 880: 873: 869: 865: 861: 858: 854: 850: 846: 841: 835: 832: 829: 825: 803: 802: 801: 790: 785: 780: 775: 770: 766: 762: 756: 753: 720: 719: 710: 708: 697: 694: 691: 687: 684: 681: 678: 675: 672: 669: 666: 663: 660: 655: 652: 648: 644: 641: 638: 634: 629: 623: 620: 617: 613: 609: 606: 603: 600: 597: 594: 591: 588: 552:Main article: 549: 546: 515: 511: 491: 490: 474: 471: 468: 463: 458: 454: 447: 443: 437: 434: 431: 428: 423: 419: 388: 387: 376: 373: 370: 366: 363: 360: 357: 351: 348: 345: 341: 334: 331: 327: 323: 320: 317: 313: 308: 302: 299: 296: 292: 286: 283: 278: 275: 272: 269: 266: 263: 260: 257: 212:Main article: 209: 206: 130: 129: 118: 115: 112: 108: 105: 102: 99: 96: 93: 90: 87: 84: 81: 78: 75: 72: 69: 66: 63: 60: 57: 54: 9: 6: 4: 3: 2: 3589: 3578: 3577:Real analysis 3575: 3573: 3570: 3568: 3565: 3564: 3562: 3551: 3547: 3546: 3538: 3533: 3532: 3523: 3519: 3515: 3511: 3507: 3505:0-691-08079-8 3501: 3497: 3493: 3492:Princeton, NJ 3489: 3488: 3483: 3479: 3476: 3475:3-540-15967-3 3472: 3467: 3463: 3459: 3455: 3451: 3449:0-387-15967-3 3445: 3441: 3437: 3436:New York City 3433: 3429: 3425: 3424: 3419: 3415: 3411: 3407: 3403: 3399: 3395: 3391: 3387: 3383: 3382:New York City 3379: 3375: 3371: 3367: 3363: 3359: 3356: 3351: 3347: 3343: 3339: 3335: 3331: 3327: 3323: 3319: 3315: 3311: 3307: 3305:0-521-42001-6 3301: 3297: 3293: 3289: 3285: 3281: 3277: 3273: 3269: 3265: 3261: 3257: 3253: 3249: 3245: 3241: 3237: 3236: 3231: 3227: 3223: 3219: 3215: 3211: 3207: 3203: 3199: 3194: 3189: 3186:(1): 85–139, 3185: 3181: 3180: 3175: 3171: 3167: 3166: 3151: 3143: 3136: 3134: 3132: 3120: 3116: 3107: 3104: 3103: 3094: 3090: 3086: 3070: 3062: 3058: 3049: 3045: 3037: 3034: 3013: 3009: 3002: 2995: 2976: 2972: 2967: 2963: 2956: 2952: 2947: 2939: 2937: 2932: 2925: 2921: 2917: 2913: 2909: 2904: 2902: 2897: 2893: 2889: 2885: 2881: 2877: 2873: 2869: 2865: 2861: 2857: 2836: 2833: 2829: 2825: 2822: 2818: 2814: 2811: 2804: 2793: 2789: 2780: 2776: 2769: 2751: 2747: 2738: 2734: 2723: 2720: 2716: 2708: 2707: 2706: 2704: 2700: 2696: 2692: 2688: 2684: 2680: 2676: 2673: 2669: 2664: 2660: 2656: 2653: −  2652: 2648: 2644: 2640: 2636: 2632: 2628: 2624: 2620: 2616: 2612: 2608: 2604: 2599: 2597: 2593: 2589: 2581: 2577: 2571: 2569: 2565: 2560: 2543: 2536: 2532: 2523: 2517: 2514: 2507: 2503: 2491: 2485: 2475: 2474: 2473: 2471: 2467: 2463: 2459: 2455: 2445: 2444: 2440: 2436: 2417: 2414: 2411: 2407: 2404: 2397: 2391: 2385: 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1353: 1341: 1335: 1325: 1322: 1319: 1311: 1303: 1300: 1296: 1290: 1287: 1284: 1272: 1271: 1270: 1268: 1264: 1245: 1242: 1237: 1233: 1229: 1224: 1220: 1210: 1207: 1204: 1201: 1198: 1191: 1185: 1178: 1174: 1170: 1162: 1154: 1149: 1145: 1140: 1132: 1131: 1130: 1128: 1124: 1120: 1101: 1098: 1091: 1085: 1079: 1073: 1068: 1065: 1057: 1048: 1040: 1036: 1029: 1021: 1015: 1009: 1003: 997: 986: 985: 984: 983: 980:given by the 979: 975: 971: 970: 964: 962: 958: 954: 933: 930: 927: 924: 921: 909: 903: 900: 894: 891: 888: 882: 867: 859: 856: 848: 839: 833: 830: 827: 815: 814: 812: 808: 804: 783: 764: 760: 751: 741: 740: 739: 735: 731: 727: 726: 725: 718: 711: 709: 695: 692: 689: 682: 676: 670: 667: 664: 658: 653: 650: 642: 639: 636: 627: 621: 615: 607: 601: 592: 586: 579: 578: 575: 573: 569: 565: 561: 555: 545: 543: 539: 535: 531: 513: 509: 500: 496: 472: 469: 466: 456: 445: 441: 435: 429: 421: 417: 409: 408: 407: 405: 401: 397: 393: 374: 371: 368: 361: 355: 349: 346: 343: 339: 332: 329: 321: 318: 315: 306: 300: 294: 284: 281: 276: 270: 261: 255: 248: 247: 246: 244: 240: 236: 232: 228: 224: 221: 215: 205: 203: 199: 195: 191: 187: 183: 179: 175: 171: 167: 163: 159: 156: =  155: 151: 147: 144: →  143: 139: 135: 116: 113: 110: 103: 97: 91: 88: 85: 79: 76: 73: 67: 58: 52: 45: 44: 43: 42: 38: 34: 30: 19: 3549: 3543: 3486: 3482:Stein, Elias 3422: 3365: 3341: 3337: 3295: 3239: 3233: 3183: 3177: 3150: 3141: 3119: 3092: 3088: 2930: 2923: 2919: 2915: 2911: 2907: 2905: 2900: 2895: 2891: 2890:. Denote by 2887: 2883: 2879: 2875: 2871: 2867: 2863: 2859: 2855: 2853: 2702: 2698: 2694: 2690: 2686: 2682: 2678: 2674: 2671: 2667: 2662: 2658: 2654: 2650: 2646: 2642: 2638: 2634: 2630: 2626: 2622: 2618: 2614: 2610: 2606: 2602: 2600: 2595: 2591: 2587: 2585: 2579: 2575: 2567: 2563: 2561: 2558: 2469: 2465: 2461: 2460:is called a 2457: 2453: 2451: 2442: 2438: 2434: 2432: 2299: 2295: 2291: 2290: 1592: 1588: 1577: 1572: 1568: 1564: 1560: 1557: 1547: 1545: 1537: 1385: 1383: 1380: 1267:odd function 1262: 1260: 1127:cancellation 1126: 1122: 1116: 977: 967: 965: 960: 956: 952: 950: 810: 806: 737: 729: 723: 712: 571: 563: 559: 557: 541: 537: 533: 529: 498: 494: 492: 403: 399: 395: 389: 242: 238: 234: 230: 226: 222: 217: 201: 197: 193: 189: 185: 181: 177: 173: 169: 165: 161: 157: 153: 145: 141: 137: 133: 131: 32: 26: 3292:Meyer, Yves 3230:Zygmund, A. 3174:Zygmund, A. 1558:A function 972:) with the 29:mathematics 3561:Categories 3522:0207.13501 3466:0612.47024 3432:Heidelberg 3410:0129.07701 3322:0916.42023 3280:0072.11501 3218:0047.10201 3163:References 2705:such that 2685:) for all 1129:condition 976:p.v.  807:smoothness 497:= 1, ..., 3390:Frankfurt 3378:Edinburgh 3256:0002-9327 3202:0001-5962 2864:accretive 2834:− 2823:≤ 2790:ψ 2777:τ 2748:φ 2735:τ 2721:∫ 2582:) theorem 2528:‖ 2521:‖ 2515:≤ 2499:‖ 2483:‖ 2433:whenever 2359:∬ 2313:∫ 2254:− 2227:− 2196:≤ 2180:− 2159:δ 2128:− 2106:− 2084:δ 2066:− 2049:≤ 2018:− 1955:− 1928:− 1897:≤ 1881:− 1860:δ 1834:− 1807:− 1785:δ 1767:− 1750:≤ 1719:− 1653:− 1636:≤ 1488:≤ 1468:∇ 1430:∖ 1402:∈ 1360:≤ 1297:∫ 1217:∀ 1141:∫ 1074:ϕ 1069:ϵ 1049:∫ 1033:→ 1030:ϵ 1016:ϕ 928:≤ 901:− 892:− 840:∫ 831:≠ 769:∞ 761:∈ 755:^ 668:− 654:ε 640:− 628:∫ 619:→ 616:ε 347:− 333:ε 319:− 307:∫ 298:→ 295:ε 285:π 77:∫ 3484:(1970), 3364:(1965), 3332:(1948), 3294:(1997), 3100:See also 3087:, where 2882:for all 2234:′ 2187:′ 2135:′ 2073:′ 2037:′ 1951:′ 1888:′ 1830:′ 1774:′ 1732:′ 1579:Calderón 1563: : 566:that is 150:singular 136: : 3514:0290095 3458:0867687 3402:0185399 3355:Russian 3350:0027429 3314:1456993 3272:0084633 3264:2372517 3210:0052553 1583:Zygmund 528:is the 168:,  3520:  3512:  3502:  3473:  3464:  3456:  3446:  3428:Berlin 3408:  3400:  3374:London 3370:Oxford 3348:  3320:  3312:  3302:  3278:  3270:  3262:  3254:  3216:  3208:  3200:  3083:is in 3031:is in 2657:) and 2617:  1585:kernel 1265:is an 1214:  493:where 237:) for 140:× 3540:(PDF) 3386:Paris 3260:JSTOR 3112:Notes 501:and 406:with 3500:ISBN 3471:ISBN 3444:ISBN 3353:(in 3300:ISBN 3252:ISSN 3198:ISSN 2929:and 2906:The 2858:and 2693:and 2586:The 2574:The 2437:and 1320:< 1304:< 1288:> 1243:> 1171:< 1155:< 1066:> 857:> 805:The 730:size 728:The 651:> 330:> 3518:Zbl 3462:Zbl 3406:Zbl 3338:UMN 3318:Zbl 3276:Zbl 3244:doi 3214:Zbl 3188:doi 3085:BMO 3033:BMO 2886:in 2689:in 2609:on 2302:if 2209:max 1910:max 1281:sup 1121:on 1026:lim 824:sup 736:of 612:lim 570:on 536:in 291:lim 241:in 204:). 148:is 27:In 3563:: 3550:45 3548:. 3542:. 3516:, 3510:MR 3508:, 3494:: 3477:). 3460:, 3454:MR 3452:, 3438:: 3426:, 3404:, 3398:MR 3392:: 3357:). 3346:MR 3340:, 3336:, 3316:, 3310:MR 3308:, 3290:; 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Index

Calderón–Zygmund kernel
mathematics
harmonic analysis
integral operator
singular
Hilbert transform
Hilbert transform
Riesz transforms
Singular integral operators of convolution type
locally integrable
Fourier transform
1
tempered distribution
principal value integral
Fourier multiplier
odd function
Calderón
Zygmund
BMO
BMO
Singular integral operators on closed curves



Calderon, A. P.
Zygmund, A.
Acta Mathematica
doi
10.1007/BF02392130
ISSN

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