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Artin billiard

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36: 985: 458: 617: 706: 789: 269: 883: 824: 190: 871: 212: 510: 537: 341: 309:
version of Artin's billiard is also exactly solvable. The eigenvalue spectrum consists of a bound state and a continuous spectrum above the energy
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The motion studied is that of a free particle sliding frictionlessly, namely, one having the
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In the case of the Artin billiards, the metric is given by the canonical Poincaré metric
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on the manifold. Because this is the free-particle Hamiltonian, the solution to the
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The system is notable in that it is an exactly solvable system that is
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E. Artin, "Ein mechanisches System mit quasi-ergodischen Bahnen",
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Type of a dynamical billiard first studied by Emil Artin in 1924
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on the upper half-plane. The non-compact Riemann surface
453:{\displaystyle H(p,q)={\frac {1}{2m}}p_{i}p_{j}g^{ij}(q)} 938: 886: 836: 800: 735: 631: 552: 518: 473: 371: 315: 228: 198: 165: 60:. Unsourced material may be challenged and removed. 979: 865: 818: 783: 700: 611: 531: 504: 452: 335: 263: 206: 184: 612:{\displaystyle p_{i}=mg_{ij}{\frac {dq^{j}}{dt}}} 279:of the modular group with the sides identified. 701:{\displaystyle ds^{2}=g_{ij}(q)\,dq^{i}\,dq^{j}} 1001:. This is the same manifold, when taken as the 784:{\displaystyle ds^{2}={\frac {dy^{2}}{y^{2}}}} 8: 1024:Abh. Math. Sem. d. Hamburgischen Universität 264:{\displaystyle \Gamma =PSL(2,\mathbb {Z} )} 962: 953: 937: 936: 930: 885: 856: 855: 835: 808: 802: 801: 799: 773: 762: 752: 743: 734: 692: 684: 678: 670: 652: 639: 630: 592: 582: 573: 557: 551: 523: 517: 478: 472: 432: 422: 412: 393: 370: 325: 314: 254: 253: 227: 200: 199: 197: 171: 167: 166: 164: 120:Learn how and when to remove this message 275:. It can be viewed as the motion on the 819:{\displaystyle {\mathcal {H}}/\Gamma } 156:of a free particle on the non-compact 512:are the coordinates on the manifold, 185:{\displaystyle \mathbb {H} /\Gamma ,} 7: 58:adding citations to reliable sources 866:{\displaystyle PSL(2,\mathbb {Z} )} 717:Hamilton-Jacobi equations of motion 813: 294:. As such, it is an example of an 229: 176: 25: 997:The manifold has, of course, one 34: 45:needs additional citations for 950: 944: 860: 846: 667: 661: 447: 441: 387: 375: 258: 244: 1: 1005:, that is the space on which 467:is the mass of the particle, 302:for analysis of the system. 207:{\displaystyle \mathbb {H} } 505:{\displaystyle q^{i},i=1,2} 1065: 152:in 1924. It describes the 719:are simply given by the 981: 875:Möbius transformations 867: 820: 785: 702: 613: 533: 506: 454: 337: 265: 208: 186: 982: 868: 821: 786: 703: 614: 534: 532:{\displaystyle p_{i}} 507: 455: 338: 336:{\displaystyle E=1/4} 298:. Artin's paper used 266: 209: 187: 884: 834: 798: 733: 629: 550: 516: 471: 369: 313: 226: 196: 163: 54:improve this article 992:fundamental domain 977: 942: 863: 816: 781: 698: 609: 529: 502: 450: 333: 307:quantum mechanical 277:fundamental domain 261: 204: 182: 146:dynamical billiard 1030:(1924) pp170-175. 1011:modular functions 994:for this action. 970: 941: 779: 723:on the manifold. 607: 541:conjugate momenta 406: 300:symbolic dynamics 286:: it is not only 218:endowed with the 148:first studied by 130: 129: 122: 104: 16:(Redirected from 1056: 1003:complex manifold 986: 984: 983: 978: 976: 972: 971: 963: 958: 954: 943: 939: 920: 872: 870: 869: 864: 859: 825: 823: 822: 817: 812: 807: 806: 790: 788: 787: 782: 780: 778: 777: 768: 767: 766: 753: 748: 747: 707: 705: 704: 699: 697: 696: 683: 682: 660: 659: 644: 643: 618: 616: 615: 610: 608: 606: 598: 597: 596: 583: 581: 580: 562: 561: 538: 536: 535: 530: 528: 527: 511: 509: 508: 503: 483: 482: 459: 457: 456: 451: 440: 439: 427: 426: 417: 416: 407: 405: 394: 349:Bessel functions 342: 340: 339: 334: 329: 284:strongly chaotic 270: 268: 267: 262: 257: 216:upper half-plane 213: 211: 210: 205: 203: 191: 189: 188: 183: 175: 170: 125: 118: 114: 111: 105: 103: 69:"Artin billiard" 62: 38: 30: 21: 1064: 1063: 1059: 1058: 1057: 1055: 1054: 1053: 1034: 1033: 1019: 1007:elliptic curves 935: 931: 910: 897: 893: 882: 881: 832: 831: 828:symmetric space 796: 795: 769: 758: 754: 739: 731: 730: 688: 674: 648: 635: 627: 626: 599: 588: 584: 569: 553: 548: 547: 519: 514: 513: 474: 469: 468: 428: 418: 408: 398: 367: 366: 357: 311: 310: 224: 223: 220:PoincarĂ© metric 194: 193: 161: 160: 158:Riemann surface 154:geodesic motion 144:is a type of a 126: 115: 109: 106: 63: 61: 51: 39: 28: 23: 22: 18:Artin billiards 15: 12: 11: 5: 1062: 1060: 1052: 1051: 1049:Ergodic theory 1046: 1036: 1035: 1032: 1031: 1018: 1015: 988: 987: 975: 969: 966: 961: 957: 952: 949: 946: 934: 929: 926: 923: 919: 916: 913: 909: 906: 903: 900: 896: 892: 889: 862: 858: 854: 851: 848: 845: 842: 839: 815: 811: 805: 792: 791: 776: 772: 765: 761: 757: 751: 746: 742: 738: 709: 708: 695: 691: 687: 681: 677: 673: 669: 666: 663: 658: 655: 651: 647: 642: 638: 634: 620: 619: 605: 602: 595: 591: 587: 579: 576: 572: 568: 565: 560: 556: 526: 522: 501: 498: 495: 492: 489: 486: 481: 477: 461: 460: 449: 446: 443: 438: 435: 431: 425: 421: 415: 411: 404: 401: 397: 392: 389: 386: 383: 380: 377: 374: 356: 353: 345:wave functions 332: 328: 324: 321: 318: 290:, but is also 260: 256: 252: 249: 246: 243: 240: 237: 234: 231: 202: 181: 178: 174: 169: 142:Artin billiard 128: 127: 110:September 2008 42: 40: 33: 26: 24: 14: 13: 10: 9: 6: 4: 3: 2: 1061: 1050: 1047: 1045: 1042: 1041: 1039: 1029: 1025: 1021: 1020: 1016: 1014: 1013:are studied. 1012: 1008: 1004: 1000: 995: 993: 973: 967: 964: 959: 955: 947: 932: 927: 924: 921: 917: 914: 911: 907: 904: 901: 898: 894: 890: 887: 880: 879: 878: 876: 852: 849: 843: 840: 837: 829: 809: 774: 770: 763: 759: 755: 749: 744: 740: 736: 729: 728: 727: 724: 722: 718: 714: 713:metric tensor 693: 689: 685: 679: 675: 671: 664: 656: 653: 649: 645: 640: 636: 632: 625: 624: 623: 603: 600: 593: 589: 585: 577: 574: 570: 566: 563: 558: 554: 546: 545: 544: 542: 524: 520: 499: 496: 493: 490: 487: 484: 479: 475: 466: 444: 436: 433: 429: 423: 419: 413: 409: 402: 399: 395: 390: 384: 381: 378: 372: 365: 364: 363: 362: 354: 352: 350: 347:are given by 346: 330: 326: 322: 319: 316: 308: 303: 301: 297: 293: 292:strong mixing 289: 285: 280: 278: 274: 273:modular group 250: 247: 241: 238: 235: 232: 221: 217: 179: 172: 159: 155: 151: 147: 143: 139: 135: 124: 121: 113: 102: 99: 95: 92: 88: 85: 81: 78: 74: 71: â€“  70: 66: 65:Find sources: 59: 55: 49: 48: 43:This article 41: 37: 32: 31: 19: 1044:Chaotic maps 1027: 1023: 996: 989: 793: 725: 710: 621: 464: 462: 358: 304: 281: 141: 131: 116: 107: 97: 90: 83: 76: 64: 52:Please help 47:verification 44: 877:. 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Index

Artin billiards

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"Artin billiard"
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mathematics
physics
dynamical billiard
Emil Artin
geodesic motion
Riemann surface
upper half-plane
Poincaré metric
modular group
fundamental domain
strongly chaotic
ergodic
strong mixing
Anosov flow
symbolic dynamics
quantum mechanical
wave functions
Bessel functions

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