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Subshift of finite type

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is an image of a subshift of finite type where different edges of the transition graph may be mapped to the same symbol. For example, if one only watches the output from a hidden Markov chain, then the output appears to be a sofic system. It may be regarded as the set of labellings of paths through
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is then any subspace of the full shift that is shift-invariant (that is, a subspace that is invariant under the action of the shift operator), non-empty, and closed for the product topology defined below. Some subshifts can be characterized by a transition matrix, as above; such subshifts are then
1826: 1346: 2968: 1137: 1603:), with certain nearest-neighbor configurations excluded. Interacting Ising models are defined as subshifts together with a continuous function of the configuration space (continuous with respect to the product topology, defined below); the 2824: 2032: 2697: 728:
Conversely, there exists a space of subshifts on 6 symbols, projected to subshifts on 2 symbols, such that any Markov measure on the smaller subshift has a preimage measure that is not Markov of any order (Example 2.6 ).
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A variety of different metrics can be defined on a shift space. One can define a metric on a shift space by considering two points to be "close" if they have many initial symbols in common; this is the
276: 2503: 1176: 2847: 1425: 1445:: there is a sequence of edges from any one vertex to any other vertex. It is precisely transitive subshifts of finite type which correspond to dynamical systems with orbits that are dense. 3174: 723: 149: 984: 192:. It consists of sequences whose transitions between consecutive letters are only those allowed by the graph. For this example, the subshift consists of only three one-sided sequences: 2353: 443: 331:
and an invariant distribution on the states, we can impose a probability measure on the set of subshifts. For example, consider the Markov chain given on the left on the states
2073: 1871: 1662: 2191: 2143: 2106: 778: 190: 529: 375: 2423: 483: 305: 663: 96: 636: 610: 581: 555: 3223: 2712: 1884: 2542: 1456:: it has a graph with an edge that connects every vertex to every other vertex; that is, all of the entries of the adjacency matrix are 1. The full 2995: 3491: 1821:{\displaystyle V^{\mathbb {Z} }=\prod _{n\in \mathbb {Z} }V=\{x=(\ldots ,x_{-1},x_{0},x_{1},\ldots ):x_{k}\in V\;\forall k\in \mathbb {Z} \}} 2235: 3540: 3451: 3427: 3385: 3349: 3407: 1604: 1341:{\displaystyle \Sigma _{A}=\left\{(\ldots ,x_{-1},x_{0},x_{1},\ldots ):x_{j}\in V,A_{x_{j}x_{j+1}}=1,j\in \mathbb {Z} \right\}.} 3582: 3572: 195: 3529:
Symbolic Dynamics and Its Applications: American Mathematical Society, Short Course, January 4-5, 2002, San Diego, California
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A (one-sided) shift of finite type is the set of all sequences, infinite on one end only, that can be made up of the letters
2963:{\displaystyle \zeta (z)=\exp \left(\sum _{n=1}^{\infty }{\Bigl |}{\textrm {Fix}}(T^{n}){\Bigr |}{\frac {z^{n}}{n}}\right),} 2835: 3532: 3483: 2703: 308: 1364: 1132:{\displaystyle \Sigma _{A}^{+}=\left\{(x_{0},x_{1},\ldots ):x_{j}\in V,A_{x_{j}x_{j+1}}=1,j\in \mathbb {N} \right\}.} 3224:
Sofic Measures: Characterizations of Hidden Markov Chains by Linear Algebra, Formal Languages, and Symbolic Dynamics
3104: 3587: 3443: 3341: 1442: 668: 101: 3577: 2982: 3479: 1578: 328: 1526: 557:, and this projection also projects the probability measure down to a probability measure on the subshifts on 2301: 3567: 3195: 1615: 1567: 151:. A (two-sided) shift of finite type is similar, but consists of sequences that are infinite on both ends. 1588:
is defined to be the set of all infinite concatenations of some fixed finite collection of finite words.
2231: 1608: 1510: 1465: 380: 278:. Similarly, the two-sided subshift described by this graph consists of only three two-sided sequences. 2046: 1844: 1635: 2167: 2119: 2082: 1546: 754: 725:, meaning that the observable part of the system can be affected by something infinitely in the past. 157: 3369: 1542: 1538: 1534: 1167: 968: 281:
Other directed graphs on the same letters produce other subshifts. For example, adding another arrow
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maps a sequence in the one- or two-sided shift to another by shifting all symbols to the left, i.e.
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obtained in this way. If the sequence extends to infinity in only one direction, it is called a
448: 3531:. Proceedings of symposia in applied mathematics: AMS short course lecture notes. Vol. 60. 947:
on such sequences; it plays the role of the time-evolution operator of the dynamical system. A
3422:, Tim Bedford, Michael Keane and Caroline Series, Eds. Oxford University Press, Oxford (1991). 3536: 3506: 3487: 3447: 3423: 3381: 3345: 3185: 3091: 1836: 798: 43: 39: 2114:
union of cylinder sets. Every open set in the subshift is the intersection of an open set of
3546: 3457: 3391: 1627: 1571: 1506: 1461: 860: 806: 638:, not even multiple orders. Intuitively, this is because if one observes a long sequence of 284: 641: 69: 3550: 3461: 3402: 3395: 3377: 3227:- Karl Petersen, Mathematics 210, Spring 2006, University of North Carolina at Chapel Hill 3190: 1563: 1518: 615: 589: 560: 534: 17: 3282: 1522: 1514: 1352: 944: 868: 787: 307:
to the graph produces a subshift that, instead of containing three sequences, contains
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called subshifts of finite type. Often, subshifts of finite type are called simply
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runs over the closed orbits. For subshifts of finite type, the zeta function is a
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of the graph, and the sequence can be either one-sided or two-sided infinite. Let
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The hidden part of a hidden Markov model, whose observable states is non-Markovian.
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A subshift can be defined by a directed graph on these letters, such as the graph
2819:{\displaystyle s_{\mu }=-\sum _{i=1}^{n}\pi _{i}\sum _{j=1}^{n}p_{ij}\log p_{ij}} 2027:{\displaystyle C_{t}=\{x\in V^{\mathbb {Z} }:x_{t}=a_{0},\ldots ,x_{t+s}=a_{s}\}} 1591:
Subshifts of finite type are identical to free (non-interacting) one-dimensional
3290: 1600: 1592: 55: 31: 2692:{\displaystyle \mu (C_{t})=\pi _{a_{0}}p_{a_{0},a_{1}}\cdots p_{a_{s-1},a_{s}}} 2196: 2038: 818: 3076:{\displaystyle \zeta (z)=\prod _{\gamma }\left(1-z^{|\gamma |}\right)^{-1}\ } 2111: 2230:
A subshift of finite type may be endowed with any one of several different
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are isomorphic to subshifts of finite type; examples include systems with
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Subshifts may be quantized in a certain way, leading to the idea of the
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Clearly this map is only invertible in the case of the two-sided shift.
3200: 1566:: a subshift of finite type then corresponds to an automaton which is 586:
The curious thing is that the probability measure on the subshifts on
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Context-free systems are defined analogously, and are generated by
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This is the space of all sequences of symbols such that the symbol
3250: 3372:; Ferenczi, SĂ©bastien; Mauduit, Christian; Siegel, A. (eds.). 1875:
which induces the topology of the subshift, is the family of
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Grammatical Complexity and One-Dimensional Dynamical Systems
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with the subshift. With respect to this topology, the shift
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Hidden Markov processes in the context of symbolic dynamics
271:{\displaystyle ABCABC\cdots ,BCABCA\cdots ,CABCAB\cdots } 3376:. Lecture Notes in Mathematics. Vol. 1794. Berlin: 3374:
Substitutions in dynamics, arithmetics and combinatorics
2215:. In fact, both the one- and two-sided shift spaces are 3420:
Ergodic Theory, Symbolic Dynamics and Hyperbolic Spaces
2498:{\displaystyle \sum _{i=1}^{n}\pi _{i}p_{ij}=\pi _{j}.} 3505:. Directions in Chaos. Vol. 6. World Scientific. 2395: 1611:
are explicitly expressible in terms of this function.
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Ordinary Differential Equations and Dynamical Systems
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A subshift has a natural topology, derived from the
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Strictly Ergodic Subshifts and Associated Operators
978:Formally, one may define the sequences of edges as 665:, then one would become increasingly sure that the 3408:Subshifts of Finite Type, Sofic Systems and Graphs 3168: 3075: 2962: 2818: 2691: 2497: 2417: 2347: 2185: 2137: 2100: 2067: 2026: 1865: 1820: 1656: 1419: 1340: 1131: 772: 717: 657: 630: 604: 575: 549: 523: 477: 437: 369: 299: 270: 184: 143: 90: 2930: 2900: 2155:; that is, with respect to this topology, it is 1420:{\displaystyle \displaystyle (T(x))_{j}=x_{j+1}.} 3283:Ergodic Theory: Basic Examples and Constructions 3126: 2508:A Markov chain, as defined above, is said to be 42:, and in particular are the objects of study in 3439:An introduction to symbolic dynamics and coding 893:the set of edges containing the directed edge 3287:Encyclopedia of Complexity and Systems Science 3169:{\displaystyle \zeta (z)=(\det(I-zA))^{-1}\ .} 3291:https://doi.org/10.1007/978-0-387-30440-3_177 718:{\displaystyle Pr(A|B^{n})\to {\frac {2}{3}}} 144:{\displaystyle AAA\cdots ,ABAB\cdots ,\dots } 27:Type of shift space studied in ergodic theory 8: 2021: 1936: 1815: 1715: 782:of all bi-infinite sequences of elements of 3416:Ergodic theory and subshifts of finite type 3240:Boyle, Mike; Petersen, Karl (2010-01-13), 1800: 3281:Matthew Nicol and Karl Petersen, (2009) " 3249: 3151: 3106: 3061: 3049: 3041: 3040: 3018: 2997: 2941: 2935: 2929: 2928: 2919: 2906: 2905: 2899: 2898: 2892: 2881: 2849: 2807: 2788: 2778: 2767: 2757: 2747: 2736: 2720: 2714: 2681: 2662: 2657: 2642: 2629: 2624: 2612: 2607: 2588: 2569: 2556: 2544: 2536:of a cylinder set may then be defined by 2486: 2470: 2460: 2450: 2439: 2433: 2403: 2394: 2330: 2320: 2309: 2303: 2177: 2176: 2175: 2169: 2129: 2128: 2127: 2121: 2092: 2091: 2090: 2084: 2056: 2055: 2054: 2048: 2015: 1996: 1977: 1964: 1951: 1950: 1949: 1924: 1905: 1892: 1886: 1854: 1853: 1852: 1846: 1811: 1810: 1788: 1766: 1753: 1737: 1703: 1702: 1695: 1682: 1681: 1680: 1674: 1645: 1644: 1643: 1637: 1401: 1388: 1366: 1326: 1325: 1296: 1286: 1281: 1262: 1240: 1227: 1211: 1184: 1178: 1117: 1116: 1087: 1077: 1072: 1053: 1031: 1018: 997: 992: 986: 764: 763: 762: 756: 705: 693: 684: 670: 649: 643: 617: 591: 562: 536: 515: 502: 490: 469: 456: 450: 445:. If we "forget" the distinction between 424: 410: 396: 382: 361: 348: 336: 286: 197: 159: 103: 71: 2989:-fold shift. It has a product formula 485:, we project this space of subshifts on 318: 3212: 2706:with relation to the Markov measure is 2348:{\displaystyle \sum _{j=1}^{n}p_{ij}=1} 3336:Brin, Michael; Stuck, Garrett (2002). 3309: 3307: 1533:(this is the first system shown to be 967:subshift of finite type, and if it is 3436:Lind, Douglas; Marcus, Brian (1995). 839:is the set of finite subsequences of 7: 3418:, (1991), appearing as Chapter 2 in 3235: 3233: 3218: 3216: 1433:A subshift of finite type is called 867:Using these elements we construct a 612:is not created by a Markov chain on 2236:measure-preserving dynamical system 1480:is understood to refer to the full 935:it is meant that the sequence is a 531:into another space of subshifts on 2893: 2238:. A common object of study is the 1801: 1181: 989: 438:{\displaystyle \pi =(2/7,4/7,1/7)} 58:are the subshifts of finite type. 25: 3338:Introduction to Dynamical Systems 2512:with the shift of finite type if 2068:{\displaystyle V^{\mathbb {Z} }.} 1866:{\displaystyle V^{\mathbb {Z} },} 1657:{\displaystyle V^{\mathbb {Z} },} 1511:transverse homoclinic connections 1448:An important special case is the 3527:Williams, Susan G., ed. (2004). 2186:{\displaystyle V^{\mathbb {Z} }} 2138:{\displaystyle V^{\mathbb {Z} }} 2101:{\displaystyle V^{\mathbb {Z} }} 773:{\displaystyle V^{\mathbb {Z} }} 185:{\displaystyle A\to B\to C\to A} 1839:. A basis for the topology of 3148: 3144: 3129: 3123: 3117: 3111: 3050: 3042: 3008: 3002: 2925: 2912: 2860: 2854: 2597: 2594: 2562: 2549: 2246:to the topology of the shift. 1930: 1898: 1778: 1724: 1385: 1381: 1375: 1369: 1252: 1198: 1146:can be followed by the symbol 1043: 1011: 702: 699: 685: 678: 432: 390: 377:, with invariant distribution 315:Markov and non-Markov measures 309:an uncountably infinite number 291: 176: 170: 164: 1: 3533:American Mathematical Society 3484:American Mathematical Society 2364:stationary probability vector 2242:, which is an extension of a 1570:. Such systems correspond to 931:sequences of edges, where by 524:{\displaystyle A,B_{1},B_{2}} 370:{\displaystyle A,B_{1},B_{2}} 3322:Brin & Stuck (2002) p.61 3313:Brin & Stuck (2002) p.60 2418:{\textstyle \sum \pi _{i}=1} 832:and the associated language 1599:-letter generalizations of 927:be the set of all infinite 478:{\displaystyle B_{1},B_{2}} 3604: 3444:Cambridge University Press 3342:Cambridge University Press 1460:-shift corresponds to the 951:is then defined as a pair 54:. The most widely studied 3368:Pytheas Fogg, N. (2002). 3301:Pytheas Fogg (2002) p.205 2836:Artin–Mazur zeta function 2249:A Markov chain is a pair 2159:with continuous inverse. 1579:phrase structure grammars 1527:Prouhet–Thue–Morse system 1495:topological Markov shifts 975:subshift of finite type. 745:symbols (alphabet). Let 2704:Kolmogorov–Sinai entropy 1476:By convention, the term 1170:is defined analogously: 1162:-th entry of the matrix 889:the set of vertices and 329:Markov transition matrix 36:subshifts of finite type 18:Subshifts of finite type 3196:Quantum finite automata 1616:quantum finite automata 1166:is 1. The space of all 949:subshift of finite type 3583:Combinatorics on words 3573:Automata (computation) 3170: 3077: 2964: 2897: 2820: 2783: 2752: 2693: 2499: 2455: 2419: 2349: 2325: 2187: 2139: 2102: 2069: 2037:The cylinder sets are 2028: 1867: 1822: 1658: 1421: 1342: 1133: 774: 719: 659: 632: 606: 577: 551: 525: 479: 439: 371: 324: 301: 300:{\displaystyle A\to C} 272: 186: 145: 92: 3171: 3078: 2965: 2877: 2821: 2763: 2732: 2694: 2500: 2435: 2420: 2350: 2305: 2195:is homeomorphic to a 2188: 2140: 2103: 2070: 2029: 1868: 1823: 1659: 1491:shifts of finite type 1422: 1343: 1168:bi-infinite sequences 1134: 775: 720: 660: 658:{\displaystyle B^{n}} 633: 607: 578: 552: 526: 480: 440: 372: 322: 302: 273: 187: 146: 93: 91:{\displaystyle A,B,C} 3501:Xie, Huimin (1996). 3105: 2996: 2848: 2713: 2543: 2432: 2393: 2302: 2234:, thus leading to a 2168: 2120: 2083: 2047: 1885: 1845: 1673: 1636: 1365: 1177: 985: 755: 669: 642: 616: 590: 561: 535: 489: 449: 381: 335: 285: 196: 158: 102: 70: 52:finite state machine 2840:formal power series 1002: 945:left shift operator 741:be a finite set of 631:{\displaystyle A,B} 605:{\displaystyle A,B} 576:{\displaystyle A,B} 550:{\displaystyle A,B} 62:Motivating examples 3414:Michael S. Keane, 3166: 3073: 3023: 2960: 2838:is defined as the 2816: 2689: 2495: 2415: 2345: 2257:consisting of the 2183: 2135: 2098: 2077:Every open set in 2065: 2024: 1863: 1818: 1708: 1654: 1605:partition function 1443:strongly connected 1417: 1416: 1338: 1129: 988: 824:-invariant subset 786:together with the 770: 715: 655: 628: 602: 573: 547: 521: 475: 435: 367: 325: 297: 268: 182: 141: 88: 38:are used to model 3588:Symbolic dynamics 3493:978-0-8218-8328-0 3186:Transfer operator 3162: 3092:rational function 3072: 3014: 2950: 2909: 2259:transition matrix 1837:discrete topology 1691: 1572:regular languages 1507:dynamical systems 971:, it is called a 799:discrete topology 713: 44:symbolic dynamics 40:dynamical systems 16:(Redirected from 3595: 3578:Markov processes 3554: 3516: 3497: 3465: 3399: 3355: 3340:(2nd ed.). 3323: 3320: 3314: 3311: 3302: 3299: 3293: 3279: 3273: 3270: 3264: 3261: 3255: 3254: 3253: 3237: 3228: 3220: 3175: 3173: 3172: 3167: 3160: 3159: 3158: 3097: 3089: 3082: 3080: 3079: 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1874: 1872: 1870: 1869: 1864: 1859: 1858: 1857: 1834: 1827: 1825: 1824: 1819: 1814: 1793: 1792: 1771: 1770: 1758: 1757: 1745: 1744: 1707: 1706: 1687: 1686: 1685: 1665: 1663: 1661: 1660: 1655: 1650: 1649: 1648: 1628:product topology 1598: 1547:Toeplitz systems 1543:Sturmian systems 1521:with a positive 1519:closed manifolds 1483: 1462:Bernoulli scheme 1459: 1453: 1440: 1426: 1424: 1423: 1418: 1412: 1411: 1393: 1392: 1357: 1347: 1345: 1344: 1339: 1334: 1330: 1329: 1309: 1308: 1307: 1306: 1291: 1290: 1267: 1266: 1245: 1244: 1232: 1231: 1219: 1218: 1189: 1188: 1165: 1161: 1149: 1145: 1138: 1136: 1135: 1130: 1125: 1121: 1120: 1100: 1099: 1098: 1097: 1082: 1081: 1058: 1057: 1036: 1035: 1023: 1022: 1001: 996: 962: 942: 926: 922: 906: 902: 892: 888: 884: 866: 863:with entries in 861:adjacency matrix 859: 849: 842: 838: 831: 827: 823: 807:product topology 804: 796: 792: 785: 781: 779: 777: 776: 771: 769: 768: 767: 748: 744: 740: 724: 722: 721: 716: 714: 706: 698: 697: 688: 664: 662: 661: 656: 654: 653: 637: 635: 634: 629: 611: 609: 608: 603: 582: 580: 579: 574: 556: 554: 553: 548: 530: 528: 527: 522: 520: 519: 507: 506: 484: 482: 481: 476: 474: 473: 461: 460: 444: 442: 441: 436: 428: 414: 400: 376: 374: 373: 368: 366: 365: 353: 352: 306: 304: 303: 298: 277: 275: 274: 269: 191: 189: 188: 183: 150: 148: 147: 142: 97: 95: 94: 89: 21: 3603: 3602: 3598: 3597: 3596: 3594: 3593: 3592: 3558: 3557: 3543: 3526: 3523: 3521:Further reading 3513: 3500: 3494: 3468: 3454: 3435: 3403:Natasha Jonoska 3388: 3378:Springer-Verlag 3370:BerthĂ©, ValĂ©rie 3367: 3358:David Damanik, 3352: 3335: 3332: 3327: 3326: 3321: 3317: 3312: 3305: 3300: 3296: 3280: 3276: 3272:Xie (1996) p.22 3271: 3267: 3263:Xie (1996) p.21 3262: 3258: 3239: 3238: 3231: 3221: 3214: 3209: 3191:De Bruijn graph 3182: 3147: 3103: 3102: 3095: 3087: 3036: 3029: 3025: 3024: 2994: 2993: 2986: 2974: 2937: 2915: 2876: 2872: 2846: 2845: 2832: 2803: 2784: 2753: 2716: 2711: 2710: 2677: 2658: 2653: 2638: 2625: 2620: 2608: 2603: 2584: 2565: 2552: 2541: 2540: 2528: 2523: 2518: 2513: 2482: 2466: 2456: 2430: 2429: 2399: 2391: 2390: 2385: 2380: 2375: 2366: 2359: 2326: 2300: 2299: 2291: 2286: 2281: 2272: 2262: 2250: 2228: 2210: 2205: 2171: 2166: 2165: 2163: 2148: 2123: 2118: 2117: 2115: 2086: 2081: 2080: 2078: 2050: 2045: 2044: 2042: 2011: 1992: 1973: 1960: 1945: 1920: 1901: 1888: 1883: 1882: 1848: 1843: 1842: 1840: 1832: 1784: 1762: 1749: 1733: 1676: 1671: 1670: 1639: 1634: 1633: 1631: 1624: 1596: 1555: 1553:Generalizations 1539:strongly mixing 1515:diffeomorphisms 1503: 1481: 1474: 1457: 1451: 1438: 1397: 1384: 1363: 1362: 1355: 1292: 1282: 1277: 1258: 1236: 1223: 1207: 1197: 1193: 1180: 1175: 1174: 1163: 1151: 1147: 1143: 1083: 1073: 1068: 1049: 1027: 1014: 1010: 1006: 983: 982: 952: 940: 924: 920: 908: 907:if and only if 904: 894: 890: 886: 871: 864: 851: 847: 840: 837: 833: 829: 825: 821: 802: 794: 790: 783: 758: 753: 752: 750: 749:denote the set 746: 742: 738: 735: 689: 667: 666: 645: 640: 639: 614: 613: 588: 587: 559: 558: 533: 532: 511: 498: 487: 486: 465: 452: 447: 446: 379: 378: 357: 344: 333: 332: 317: 283: 282: 194: 193: 156: 155: 100: 99: 68: 67: 64: 28: 23: 22: 15: 12: 11: 5: 3601: 3599: 3591: 3590: 3585: 3580: 3575: 3570: 3568:Ergodic theory 3560: 3559: 3556: 3555: 3541: 3522: 3519: 3518: 3517: 3511: 3498: 3492: 3470:Teschl, Gerald 3466: 3452: 3433: 3412: 3400: 3386: 3365: 3356: 3350: 3331: 3328: 3325: 3324: 3315: 3303: 3294: 3274: 3265: 3256: 3229: 3211: 3210: 3208: 3205: 3204: 3203: 3198: 3193: 3188: 3181: 3178: 3177: 3176: 3165: 3157: 3154: 3150: 3146: 3143: 3140: 3137: 3134: 3131: 3128: 3125: 3122: 3119: 3116: 3113: 3110: 3084: 3083: 3067: 3064: 3059: 3052: 3048: 3044: 3039: 3035: 3032: 3028: 3021: 3017: 3013: 3010: 3007: 3004: 3001: 2981:is the set of 2971: 2970: 2959: 2955: 2949: 2944: 2940: 2932: 2927: 2922: 2918: 2914: 2902: 2895: 2890: 2887: 2884: 2880: 2875: 2871: 2868: 2865: 2862: 2859: 2856: 2853: 2831: 2828: 2827: 2826: 2813: 2810: 2806: 2802: 2799: 2794: 2791: 2787: 2781: 2776: 2773: 2770: 2766: 2760: 2756: 2750: 2745: 2742: 2739: 2735: 2731: 2728: 2723: 2719: 2700: 2699: 2684: 2680: 2676: 2671: 2668: 2665: 2661: 2656: 2652: 2645: 2641: 2637: 2632: 2628: 2623: 2615: 2611: 2606: 2602: 2599: 2596: 2591: 2587: 2583: 2580: 2577: 2572: 2568: 2564: 2559: 2555: 2551: 2548: 2534:Markov measure 2526: 2516: 2506: 2505: 2494: 2489: 2485: 2481: 2476: 2473: 2469: 2463: 2459: 2453: 2448: 2445: 2442: 2438: 2414: 2411: 2406: 2402: 2398: 2383: 2373: 2356: 2355: 2344: 2341: 2336: 2333: 2329: 2323: 2318: 2315: 2312: 2308: 2289: 2285:for which all 2279: 2240:Markov measure 2227: 2224: 2204: 2201: 2179: 2174: 2131: 2126: 2094: 2089: 2064: 2058: 2053: 2035: 2034: 2023: 2018: 2014: 2010: 2005: 2002: 1999: 1995: 1991: 1988: 1985: 1980: 1976: 1972: 1967: 1963: 1959: 1953: 1948: 1944: 1941: 1938: 1935: 1932: 1927: 1923: 1919: 1916: 1913: 1908: 1904: 1900: 1895: 1891: 1862: 1856: 1851: 1829: 1828: 1817: 1813: 1809: 1806: 1803: 1799: 1796: 1791: 1787: 1783: 1780: 1777: 1774: 1769: 1765: 1761: 1756: 1752: 1748: 1743: 1740: 1736: 1732: 1729: 1726: 1723: 1720: 1717: 1714: 1711: 1705: 1701: 1698: 1694: 1690: 1684: 1679: 1653: 1647: 1642: 1623: 1620: 1586:renewal system 1554: 1551: 1523:metric entropy 1502: 1499: 1473: 1470: 1428: 1427: 1415: 1410: 1407: 1404: 1400: 1396: 1391: 1387: 1383: 1380: 1377: 1374: 1371: 1353:shift operator 1349: 1348: 1337: 1333: 1328: 1324: 1321: 1318: 1315: 1312: 1305: 1302: 1299: 1295: 1289: 1285: 1280: 1276: 1273: 1270: 1265: 1261: 1257: 1254: 1251: 1248: 1243: 1239: 1235: 1230: 1226: 1222: 1217: 1214: 1210: 1206: 1203: 1200: 1196: 1192: 1187: 1183: 1140: 1139: 1128: 1124: 1119: 1115: 1112: 1109: 1106: 1103: 1096: 1093: 1090: 1086: 1080: 1076: 1071: 1067: 1064: 1061: 1056: 1052: 1048: 1045: 1042: 1039: 1034: 1030: 1026: 1021: 1017: 1013: 1009: 1005: 1000: 995: 991: 912: 869:directed graph 835: 788:shift operator 766: 761: 734: 731: 712: 709: 704: 701: 696: 692: 687: 683: 680: 677: 674: 652: 648: 627: 624: 621: 601: 598: 595: 572: 569: 566: 546: 543: 540: 518: 514: 510: 505: 501: 497: 494: 472: 468: 464: 459: 455: 434: 431: 427: 423: 420: 417: 413: 409: 406: 403: 399: 395: 392: 389: 386: 364: 360: 356: 351: 347: 343: 340: 316: 313: 311:of sequences. 296: 293: 290: 267: 264: 261: 258: 255: 252: 249: 246: 243: 240: 237: 234: 231: 228: 225: 222: 219: 216: 213: 210: 207: 204: 201: 181: 178: 175: 172: 169: 166: 163: 140: 137: 134: 131: 128: 125: 122: 119: 116: 113: 110: 107: 87: 84: 81: 78: 75: 63: 60: 48:ergodic theory 26: 24: 14: 13: 10: 9: 6: 4: 3: 2: 3600: 3589: 3586: 3584: 3581: 3579: 3576: 3574: 3571: 3569: 3566: 3565: 3563: 3552: 3548: 3544: 3542:0-8218-3157-7 3538: 3534: 3530: 3525: 3524: 3520: 3514: 3508: 3504: 3499: 3495: 3489: 3485: 3481: 3477: 3476: 3471: 3467: 3463: 3459: 3455: 3453:0-521-55124-2 3449: 3445: 3441: 3440: 3434: 3432: 3429: 3428:0-19-853390-X 3425: 3421: 3417: 3413: 3410: 3409: 3404: 3401: 3397: 3393: 3389: 3387:3-540-44141-7 3383: 3379: 3375: 3371: 3366: 3363: 3362: 3357: 3353: 3351:0-521-80841-3 3347: 3343: 3339: 3334: 3333: 3329: 3319: 3316: 3310: 3308: 3304: 3298: 3295: 3292: 3288: 3284: 3278: 3275: 3269: 3266: 3260: 3257: 3252: 3247: 3243: 3236: 3234: 3230: 3226: 3225: 3219: 3217: 3213: 3206: 3202: 3199: 3197: 3194: 3192: 3189: 3187: 3184: 3183: 3179: 3163: 3155: 3152: 3141: 3138: 3135: 3132: 3120: 3114: 3108: 3101: 3100: 3099: 3093: 3065: 3062: 3057: 3046: 3037: 3033: 3030: 3026: 3019: 3015: 3011: 3005: 2999: 2992: 2991: 2990: 2984: 2978: 2957: 2953: 2947: 2942: 2938: 2920: 2916: 2888: 2885: 2882: 2878: 2873: 2869: 2866: 2863: 2857: 2851: 2844: 2843: 2842: 2841: 2837: 2830:Zeta function 2829: 2811: 2808: 2804: 2800: 2797: 2792: 2789: 2785: 2779: 2774: 2771: 2768: 2764: 2758: 2754: 2748: 2743: 2740: 2737: 2733: 2729: 2726: 2721: 2717: 2709: 2708: 2707: 2705: 2682: 2678: 2674: 2669: 2666: 2663: 2659: 2654: 2650: 2643: 2639: 2635: 2630: 2626: 2621: 2613: 2609: 2604: 2600: 2589: 2585: 2581: 2578: 2575: 2570: 2566: 2557: 2553: 2546: 2539: 2538: 2537: 2535: 2529: 2519: 2511: 2492: 2487: 2483: 2479: 2474: 2471: 2467: 2461: 2457: 2451: 2446: 2443: 2440: 2436: 2428: 2427: 2426: 2412: 2409: 2404: 2400: 2396: 2386: 2376: 2369: 2365: 2342: 2339: 2334: 2331: 2327: 2321: 2316: 2313: 2310: 2306: 2298: 2297: 2296: 2292: 2282: 2275: 2269: 2265: 2260: 2254: 2247: 2245: 2241: 2237: 2233: 2225: 2223: 2221: 2220:metric spaces 2218: 2214: 2202: 2200: 2198: 2172: 2160: 2158: 2154: 2153:homeomorphism 2124: 2113: 2087: 2062: 2051: 2040: 2016: 2012: 2008: 2003: 2000: 1997: 1993: 1989: 1986: 1983: 1978: 1974: 1970: 1965: 1961: 1957: 1946: 1942: 1939: 1933: 1925: 1921: 1917: 1914: 1911: 1906: 1902: 1893: 1889: 1881: 1880: 1879: 1878: 1877:cylinder sets 1860: 1849: 1838: 1835:is given the 1807: 1804: 1797: 1794: 1789: 1785: 1781: 1775: 1772: 1767: 1763: 1759: 1754: 1750: 1746: 1741: 1738: 1734: 1730: 1727: 1721: 1718: 1712: 1709: 1699: 1696: 1692: 1688: 1677: 1669: 1668: 1667: 1651: 1640: 1629: 1621: 1619: 1617: 1612: 1610: 1606: 1602: 1594: 1589: 1587: 1582: 1580: 1575: 1573: 1569: 1568:deterministic 1565: 1560: 1552: 1550: 1548: 1544: 1540: 1536: 1535:weakly mixing 1532: 1531:Chacon system 1528: 1524: 1520: 1516: 1512: 1508: 1505:Many chaotic 1500: 1498: 1496: 1492: 1487: 1479: 1471: 1469: 1467: 1463: 1455: 1446: 1444: 1436: 1431: 1413: 1408: 1405: 1402: 1398: 1394: 1389: 1378: 1372: 1361: 1360: 1359: 1354: 1335: 1331: 1322: 1319: 1316: 1313: 1310: 1303: 1300: 1297: 1293: 1287: 1283: 1278: 1274: 1271: 1268: 1263: 1259: 1255: 1249: 1246: 1241: 1237: 1233: 1228: 1224: 1220: 1215: 1212: 1208: 1204: 1201: 1194: 1190: 1185: 1173: 1172: 1171: 1169: 1159: 1155: 1126: 1122: 1113: 1110: 1107: 1104: 1101: 1094: 1091: 1088: 1084: 1078: 1074: 1069: 1065: 1062: 1059: 1054: 1050: 1046: 1040: 1037: 1032: 1028: 1024: 1019: 1015: 1007: 1003: 998: 993: 981: 980: 979: 976: 974: 970: 966: 960: 956: 950: 946: 938: 934: 930: 919: 915: 911: 901: 897: 882: 878: 874: 870: 862: 858: 854: 844: 820: 816: 812: 811:symbolic flow 808: 800: 789: 759: 732: 730: 726: 710: 707: 694: 690: 681: 675: 672: 650: 646: 625: 622: 619: 599: 596: 593: 584: 570: 567: 564: 544: 541: 538: 516: 512: 508: 503: 499: 495: 492: 470: 466: 462: 457: 453: 429: 425: 421: 418: 415: 411: 407: 404: 401: 397: 393: 387: 384: 362: 358: 354: 349: 345: 341: 338: 330: 321: 314: 312: 310: 294: 288: 279: 265: 262: 259: 256: 253: 250: 247: 244: 241: 238: 235: 232: 229: 226: 223: 220: 217: 214: 211: 208: 205: 202: 199: 179: 173: 167: 161: 152: 138: 135: 132: 129: 126: 123: 120: 117: 114: 111: 108: 105: 85: 82: 79: 76: 73: 61: 59: 57: 53: 49: 45: 41: 37: 33: 19: 3528: 3502: 3474: 3438: 3430: 3419: 3415: 3406: 3373: 3359: 3337: 3318: 3297: 3286: 3277: 3268: 3259: 3241: 3222: 3085: 2983:fixed points 2976: 2972: 2833: 2701: 2533: 2524: 2514: 2509: 2507: 2381: 2371: 2367: 2363: 2357: 2287: 2277: 2273: 2267: 2263: 2258: 2252: 2248: 2244:Markov chain 2239: 2229: 2213:-adic metric 2206: 2161: 2036: 1830: 1625: 1613: 1601:Ising models 1593:Potts models 1590: 1585: 1583: 1576: 1559:sofic system 1558: 1556: 1504: 1494: 1490: 1485: 1477: 1475: 1464:without the 1449: 1447: 1434: 1432: 1429: 1350: 1157: 1153: 1150:only if the 1141: 977: 972: 964: 958: 954: 948: 932: 928: 917: 913: 909: 899: 895: 880: 876: 872: 856: 852: 845: 814: 810: 793:. We endow 736: 727: 585: 326: 280: 153: 65: 56:shift spaces 35: 29: 3289:, Springer 2039:clopen sets 1609:Hamiltonian 1484:-shift. A 1472:Terminology 32:mathematics 3562:Categories 3551:1052.37003 3512:9810223986 3480:Providence 3462:1106.37301 3396:1014.11015 3330:References 2510:compatible 2197:Cantor set 2162:The space 2157:continuous 1435:transitive 933:admissible 929:admissible 733:Definition 3411:, (2000). 3251:0907.1858 3153:− 3136:− 3109:ζ 3063:− 3047:γ 3034:− 3020:γ 3016:∏ 3000:ζ 2894:∞ 2879:∑ 2870:⁡ 2852:ζ 2801:⁡ 2765:∑ 2755:π 2734:∑ 2730:− 2722:μ 2667:− 2651:⋯ 2605:π 2579:… 2547:μ 2522:whenever 2484:π 2458:π 2437:∑ 2401:π 2397:∑ 2387:≥ 0 2307:∑ 2293:≥ 0 2112:countable 1987:… 1943:∈ 1915:… 1808:∈ 1802:∀ 1795:∈ 1776:… 1739:− 1728:… 1700:∈ 1693:∏ 1564:automaton 1323:∈ 1269:∈ 1250:… 1213:− 1202:… 1182:Σ 1114:∈ 1060:∈ 1041:… 990:Σ 973:two-sided 969:bilateral 965:one-sided 805:with the 797:with the 703:→ 385:π 292:→ 266:⋯ 242:⋯ 218:⋯ 177:→ 171:→ 165:→ 139:… 133:⋯ 115:⋯ 3472:(2012). 3364:, (2005) 3180:See also 2425:and has 2379:has all 2358:for all 2232:measures 1622:Topology 1537:but not 1501:Examples 1486:subshift 846:Now let 815:subshift 327:Given a 3201:Axiom A 2985:of the 2532:. The 2271:matrix 2226:Measure 2217:compact 2193:⁠ 2164:⁠ 2145:⁠ 2116:⁠ 2108:⁠ 2079:⁠ 2075:⁠ 2043:⁠ 1873:⁠ 1841:⁠ 1664:⁠ 1632:⁠ 1466:measure 943:be the 923:. Let 865:{0, 1}. 780:⁠ 751:⁠ 98:, like 3549:  3539:  3509:  3490:  3460:  3450:  3426:  3394:  3384:  3348:  3161:  3086:where 3071:  2973:where 2382:π 2372:π 2368:π 2362:. The 2203:Metric 1666:where 1529:, the 1525:, the 1454:-shift 850:be an 819:closed 3246:arXiv 3207:Notes 2261:, an 2151:is a 2110:is a 1478:shift 1450:full 885:with 817:is a 809:. A 3537:ISBN 3507:ISBN 3488:ISBN 3448:ISBN 3424:ISBN 3382:ISBN 3346:ISBN 2975:Fix( 2834:The 2702:The 2295:and 2255:, Ď€) 1831:and 1607:and 1545:and 1351:The 937:walk 801:and 737:Let 46:and 3547:Zbl 3458:Zbl 3392:Zbl 3285:", 3127:det 3094:of 2908:Fix 2867:exp 2798:log 2530:= 0 2520:= 0 2370:= ( 2276:= ( 2041:in 1630:on 1562:an 1541:), 1517:of 1441:is 1437:if 921:= 1 903:in 875:= ( 828:of 813:or 30:In 3564:: 3545:. 3535:. 3486:. 3482:: 3478:. 3456:. 3446:. 3442:. 3405:, 3390:. 3380:. 3344:. 3306:^ 3244:, 3232:^ 3215:^ 3098:: 2527:ij 2517:ij 2389:, 2290:ij 2280:ij 2266:Ă— 2222:. 2199:. 1618:. 1584:A 1581:. 1574:. 1557:A 1549:. 1513:, 1497:. 1468:. 1156:, 957:, 916:, 898:→ 879:, 855:Ă— 843:. 583:. 34:, 3553:. 3515:. 3496:. 3464:. 3398:. 3354:. 3248:: 3164:. 3156:1 3149:) 3145:) 3142:A 3139:z 3133:I 3130:( 3124:( 3121:= 3118:) 3115:z 3112:( 3096:z 3088:Îł 3066:1 3058:) 3051:| 3043:| 3038:z 3031:1 3027:( 3012:= 3009:) 3006:z 3003:( 2987:n 2979:) 2977:T 2958:, 2954:) 2948:n 2943:n 2939:z 2931:| 2926:) 2921:n 2917:T 2913:( 2901:| 2889:1 2886:= 2883:n 2874:( 2864:= 2861:) 2858:z 2855:( 2812:j 2809:i 2805:p 2793:j 2790:i 2786:p 2780:n 2775:1 2772:= 2769:j 2759:i 2749:n 2744:1 2741:= 2738:i 2727:= 2718:s 2683:s 2679:a 2675:, 2670:1 2664:s 2660:a 2655:p 2644:1 2640:a 2636:, 2631:0 2627:a 2622:p 2614:0 2610:a 2601:= 2598:) 2595:] 2590:s 2586:a 2582:, 2576:, 2571:0 2567:a 2563:[ 2558:t 2554:C 2550:( 2525:A 2515:p 2493:. 2488:j 2480:= 2475:j 2472:i 2468:p 2462:i 2452:n 2447:1 2444:= 2441:i 2413:1 2410:= 2405:i 2384:i 2377:) 2374:i 2360:i 2343:1 2340:= 2335:j 2332:i 2328:p 2322:n 2317:1 2314:= 2311:j 2288:p 2283:) 2278:p 2274:P 2268:n 2264:n 2253:P 2251:( 2211:p 2178:Z 2173:V 2149:T 2130:Z 2125:V 2093:Z 2088:V 2063:. 2057:Z 2052:V 2022:} 2017:s 2013:a 2009:= 2004:s 2001:+ 1998:t 1994:x 1990:, 1984:, 1979:0 1975:a 1971:= 1966:t 1962:x 1958:: 1952:Z 1947:V 1940:x 1937:{ 1934:= 1931:] 1926:s 1922:a 1918:, 1912:, 1907:0 1903:a 1899:[ 1894:t 1890:C 1861:, 1855:Z 1850:V 1833:V 1816:} 1812:Z 1805:k 1798:V 1790:k 1786:x 1782:: 1779:) 1773:, 1768:1 1764:x 1760:, 1755:0 1751:x 1747:, 1742:1 1735:x 1731:, 1725:( 1722:= 1719:x 1716:{ 1713:= 1710:V 1704:Z 1697:n 1689:= 1683:Z 1678:V 1652:, 1646:Z 1641:V 1597:n 1595:( 1482:n 1458:n 1452:n 1439:G 1414:. 1409:1 1406:+ 1403:j 1399:x 1395:= 1390:j 1386:) 1382:) 1379:x 1376:( 1373:T 1370:( 1356:T 1336:. 1332:} 1327:Z 1320:j 1317:, 1314:1 1311:= 1304:1 1301:+ 1298:j 1294:x 1288:j 1284:x 1279:A 1275:, 1272:V 1264:j 1260:x 1256:: 1253:) 1247:, 1242:1 1238:x 1234:, 1229:0 1225:x 1221:, 1216:1 1209:x 1205:, 1199:( 1195:{ 1191:= 1186:A 1164:A 1160:) 1158:q 1154:p 1152:( 1148:q 1144:p 1127:. 1123:} 1118:N 1111:j 1108:, 1105:1 1102:= 1095:1 1092:+ 1089:j 1085:x 1079:j 1075:x 1070:A 1066:, 1063:V 1055:j 1051:x 1047:: 1044:) 1038:, 1033:1 1029:x 1025:, 1020:0 1016:x 1012:( 1008:{ 1004:= 999:+ 994:A 961:) 959:T 955:Y 953:( 941:T 925:Y 918:y 914:x 910:A 905:E 900:y 896:x 891:E 887:V 883:) 881:E 877:V 873:G 857:n 853:n 848:A 841:Y 836:Y 834:L 830:X 826:Y 822:T 803:X 795:V 791:T 784:V 765:Z 760:V 747:X 743:n 739:V 711:3 708:2 700:) 695:n 691:B 686:| 682:A 679:( 676:r 673:P 651:n 647:B 626:B 623:, 620:A 600:B 597:, 594:A 571:B 568:, 565:A 545:B 542:, 539:A 517:2 513:B 509:, 504:1 500:B 496:, 493:A 471:2 467:B 463:, 458:1 454:B 433:) 430:7 426:/ 422:1 419:, 416:7 412:/ 408:4 405:, 402:7 398:/ 394:2 391:( 388:= 363:2 359:B 355:, 350:1 346:B 342:, 339:A 295:C 289:A 263:B 260:A 257:C 254:B 251:A 248:C 245:, 239:A 236:C 233:B 230:A 227:C 224:B 221:, 215:C 212:B 209:A 206:C 203:B 200:A 180:A 174:C 168:B 162:A 136:, 130:B 127:A 124:B 121:A 118:, 112:A 109:A 106:A 86:C 83:, 80:B 77:, 74:A 20:)

Index

Subshifts of finite type
mathematics
dynamical systems
symbolic dynamics
ergodic theory
finite state machine
shift spaces
an uncountably infinite number

Markov transition matrix
shift operator
discrete topology
product topology
closed
adjacency matrix
directed graph
walk
left shift operator
bilateral
bi-infinite sequences
shift operator
strongly connected
Bernoulli scheme
measure
dynamical systems
transverse homoclinic connections
diffeomorphisms
closed manifolds
metric entropy
Prouhet–Thue–Morse system

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