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Spray (mathematics)

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1321: 976: 5108: 1316:{\displaystyle {\frac {d}{ds}}{\Big |}_{s=0}{\mathcal {S}}(\gamma _{s})={\Big |}_{a}^{b}{\frac {\partial L}{\partial \xi ^{i}}}X^{i}-\int _{a}^{b}{\Big (}{\frac {\partial ^{2}L}{\partial \xi ^{j}\partial \xi ^{i}}}{\ddot {\gamma }}^{j}+{\frac {\partial ^{2}L}{\partial x^{j}\partial \xi ^{i}}}{\dot {\gamma }}^{j}-{\frac {\partial L}{\partial x^{i}}}{\Big )}X^{i}dt,} 2759: 2540: 2942: 3822: 3156: 702: 2551: 5086: 3605: 4556: 4424: 4083: 2366: 1976: 2778: 3624: 2953: 960: 537: 1752: 820: 1548: 4861: 2754:{\displaystyle dE={\Big (}{\frac {\partial ^{2}L}{\partial x^{i}\partial \xi ^{j}}}\xi ^{j}-{\frac {\partial L}{\partial x^{i}}}{\Big )}dx^{i}+\xi ^{j}{\frac {\partial ^{2}L}{\partial \xi ^{i}\partial x^{j}}}d\xi ^{i}} 1459: 4290: 3432: 4922: 2257: 1864: 3911: 4937: 3443: 3288: 2338: 4765: 4430: 4298: 2182: 2135: 4691: 1636: 2052: 3831:
for this mechanical system is a full spray. The constant speed geodesics of the underlying Finsler (or Riemannian) manifold are described by this spray for the following reasons:
3967: 2535:{\displaystyle \iota _{H}d\alpha =Y^{i}{\frac {\partial ^{2}L}{\partial \xi ^{i}\partial x^{j}}}dx^{j}-X^{i}{\frac {\partial ^{2}L}{\partial \xi ^{i}\partial x^{j}}}d\xi ^{j}} 416: 2088: 2016: 1588: 4130: 3958: 1869: 2937:{\displaystyle G^{k}(x,\xi )={\frac {g^{ki}}{2}}{\Big (}{\frac {\partial ^{2}L}{\partial \xi ^{i}\partial x^{j}}}\xi ^{j}-{\frac {\partial L}{\partial x^{i}}}{\Big )}.} 3817:{\displaystyle g_{ij}(\lambda \xi )=g_{ij}(\xi ),\quad \alpha _{i}(x,\lambda \xi )=\lambda \alpha _{i}(x,\xi ),\quad G^{i}(x,\lambda \xi )=\lambda ^{2}G^{i}(x,\xi ),} 469: 3151:{\displaystyle {\frac {d}{ds}}{\Big |}_{s=0}{\mathcal {S}}(\gamma _{s})={\Big |}_{a}^{b}\alpha _{i}X^{i}-\int _{a}^{b}g_{ik}({\ddot {\gamma }}^{k}+2G^{k})X^{i}dt,} 439: 4204: 4184: 697:{\displaystyle H_{\xi }=\xi ^{i}{\frac {\partial }{\partial x^{i}}}{\Big |}_{(x,\xi )}-2G^{i}(x,\xi ){\frac {\partial }{\partial \xi ^{i}}}{\Big |}_{(x,\xi )}.} 529: 509: 489: 863: 1641: 728: 1464: 4776: 4132:
is stationary to the action integral if and only if it is of constant speed and stationary to the length functional. The Hamiltonian vector field
1363: 96:
are precisely the tangent curves of locally length minimizing curves. Semisprays arise naturally as the extremal curves of action integrals in
4209: 3362: 4872: 2194: 1764: 3205:. Using the framework of Lagrangian mechanics one can describe these curves with spray structures. Define a Lagrangian function on 5081:{\displaystyle \epsilon |_{\xi }=\int \limits _{-\infty }^{0}e^{-s}(\Phi _{V}^{-s})_{*}(\tau \Theta V)|_{\Phi _{V}^{s}(\xi )}ds.} 3600:{\displaystyle \alpha _{i}=g_{ij}\xi ^{i},\quad F^{2}=g_{ij}\xi ^{i}\xi ^{j},\quad E=\alpha _{i}\xi ^{i}-L={\tfrac {1}{2}}F^{2}.} 3848: 5231: 3215: 3842:
is positive definite for Finsler spaces, every short enough stationary curve for the length functional is length minimizing.
4551:{\displaystyle v:T(TM\setminus 0)\to T(TM\setminus 0)\quad ;\quad v={\tfrac {1}{2}}{\big (}I+{\mathcal {L}}_{H}J{\big )}.} 4419:{\displaystyle h:T(TM\setminus 0)\to T(TM\setminus 0)\quad ;\quad h={\tfrac {1}{2}}{\big (}I-{\mathcal {L}}_{H}J{\big )},} 2296: 4730: 3330:)ξξ. Now introduce the concepts from the section above. In the Riemannian case it turns out that the fundamental tensor 5166: 5148: 5158: 2140: 2093: 5236: 4704:\0 and the adjoint structure Θ of the induced connection the horizontal part of the semi-spray can be written as 4575: 1596: 1356:). This first variation formula can be recast in a more informative form by introducing the following concepts: 2276: 4078:{\displaystyle {\mathcal {S}}(\gamma )={\frac {(b-a)\lambda ^{2}}{2}}={\frac {\ell (\gamma )^{2}}{2(b-a)}}.} 2028: 133: 159: 853:. The dynamical law is obtained from the Hamiltonian principle, which states that the time evolution γ:→ 254: 212: 163: 20: 3173:. Hence the dynamics of mechanical systems are described by semisprays arising from action integrals. 375: 97: 42: 2057: 1985: 1971:{\displaystyle g_{ij}(x,\xi )={\tfrac {\partial ^{2}L}{\partial \xi ^{i}\partial \xi ^{j}}}(x,\xi )} 1557: 4091: 3919: 3194: 831: 81: 3165:
is stationary for the action integral with fixed end points if and only if its tangent curve γ':→
4565:\0 always has a vanishing torsion tensor, which is defined as the Frölicher-Nijenhuis bracket 120:, and homogeneous torsion-free connections are in one-to-one correspondence with full sprays. 3610:
In terms of classical mechanics, the last equation states that all the energy in the system (
3306: 3198: 444: 85: 5091:
From this relation one also sees that the induced connection is homogeneous if and only if
2272: 955:{\displaystyle {\mathcal {S}}(\gamma ):=\int _{a}^{b}L(\gamma (t),{\dot {\gamma }}(t))dt} 116:. If the original connection is torsion-free it coincides with the connection induced by 421: 4189: 4169: 3182: 846: 514: 494: 474: 93: 89: 35: 5107: 1747:{\displaystyle \alpha _{\xi }=\alpha _{i}(x,\xi )dx^{i}|_{(x,\xi )}\in T_{\xi }^{*}TM} 815:{\displaystyle G^{i}(x,\lambda \xi )=\lambda ^{2}G^{i}(x,\xi ),\quad \lambda >0.\,} 49:. Usually a spray is required to be homogeneous in the sense that its integral curves 5225: 3188: 1543:{\displaystyle \alpha _{i}(x,\xi )={\tfrac {\partial L}{\partial \xi ^{i}}}(x,\xi )} 28: 4866:
of the induced non-linear connection through the ordinary differential equation
3960:
of constant speed the action integral and the length functional are related by
3618:) is in the kinetic form. Furthermore, one obtains the homogeneity properties 4856:{\displaystyle \tau ={\mathcal {L}}_{V}v={\tfrac {1}{2}}{\mathcal {L}}_{-H}J} 4292:
on the slit tangent bundle through its horizontal and vertical projections
3202: 45:
second order system of ordinary differential equations on the base manifold
1454:{\displaystyle \alpha _{\xi }=\alpha _{i}(x,\xi )dx^{i}|_{x}\in T_{x}^{*}M} 5171: 100:. Generalizing all these examples, any (possibly nonlinear) connection on 4285:{\displaystyle T(TM\setminus 0)=H(TM\setminus 0)\oplus V(TM\setminus 0)} 4927:
Therefore, the first spray invariant ε (and hence the whole semi-spray
3427:{\displaystyle F(x,\lambda \xi )=\lambda F(x,\xi ),\quad \lambda >0} 69:(ξ) in positive re-parameterizations. If this requirement is dropped, 5156:
Bucătaru, Constantinescu and Dahl relate this concept to that of the
4917:{\displaystyle {\mathcal {L}}_{V}\epsilon +\epsilon =\tau \Theta V.} 3845:
Every stationary curve for the action integral is of constant speed
5153: 2252:{\displaystyle \displaystyle E(\xi )=\alpha _{\xi }(\xi )-L(\xi )} 1859:{\displaystyle g_{\xi }=g_{ij}(x,\xi )(dx^{i}\otimes dx^{j})|_{x}} 857:
of the state of the system is stationary for the action integral
5146:
by Bucătaru and Miron. Of particular note is their concept of a
5138:
A good source for Jacobi fields of semisprays is Section 4.4,
5102: 1334:
is the variation vector field associated with the variation γ
3827:
of which the last one says that the Hamiltonian vector field
177:, if any of the three following equivalent conditions holds: 4879: 4821: 4789: 4524: 4392: 3973: 2994: 1017: 869: 4569:=. In more elementary terms the torsion can be defined as 3906:{\displaystyle F(\gamma (t),{\dot {\gamma }}(t))=\lambda } 830:
A physical system is modeled in Lagrangian mechanics by a
3913:, since the energy is automatically a constant of motion. 3437:
of the Finsler-function implies the following formulae:
5119: 3283:{\displaystyle L(x,\xi )={\tfrac {1}{2}}F^{2}(x,\xi ),} 491:
using the coordinate basis on each tangent space. Then
4807: 4497: 4365: 3573: 3241: 3169:
is an integral curve for the Hamiltonian vector field
2947:
Now the first variational formula can be rewritten as
1905: 1497: 4940: 4931:) can be recovered from the non-linear connection by 4875: 4779: 4734: 4733: 4579: 4578: 4433: 4301: 4212: 4192: 4172: 4094: 3970: 3922: 3851: 3627: 3446: 3365: 3218: 2956: 2781: 2554: 2369: 2300: 2299: 2198: 2197: 2144: 2143: 2097: 2096: 2060: 2032: 2031: 1988: 1872: 1767: 1644: 1599: 1560: 1467: 1366: 979: 866: 731: 540: 517: 497: 477: 447: 424: 378: 4770:
The first spray invariant is related to the tension
2352:) be the components of the Hamiltonian vector field 2333:{\displaystyle \displaystyle dE=-\iota _{H}d\alpha } 970:
the first variation of the action integral reads as
285:
if any of the following equivalent conditions hold:
4760:{\displaystyle \displaystyle H=\Theta V+\epsilon .} 5080: 4916: 4855: 4759: 4685: 4550: 4418: 4284: 4198: 4178: 4124: 4077: 3952: 3905: 3816: 3599: 3426: 3282: 3150: 2936: 2753: 2534: 2332: 2251: 2176: 2129: 2082: 2046: 2010: 1970: 1858: 1746: 1630: 1582: 1542: 1453: 1315: 954: 814: 696: 523: 503: 483: 463: 433: 410: 3356:). In the general case the homogeneity condition 3021: 2975: 2926: 2832: 2660: 2566: 1289: 1117: 1044: 998: 668: 589: 112:induces a torsion-free nonlinear connection on 4540: 4510: 4408: 4378: 2263:If the Legendre condition is satisfied, then 531:if it has a local representation of the form 8: 2764:so we see that the Hamiltonian vector field 2177:{\displaystyle \displaystyle g^{ij}(x,\xi )} 2130:{\displaystyle \displaystyle g_{ij}(x,\xi )} 318:is the push-forward of the multiplication λ: 4686:{\displaystyle \displaystyle T(X,Y)=J-v-v.} 2768:is a semi-spray on the configuration space 2286:corresponding to the Hamiltonian function 1631:{\displaystyle \alpha \in \Omega ^{1}(TM)} 150:) its tangent bundle. Then a vector field 5052: 5047: 5042: 5037: 5015: 5002: 4997: 4981: 4971: 4963: 4950: 4945: 4939: 4884: 4878: 4877: 4874: 4826: 4820: 4819: 4806: 4794: 4788: 4787: 4778: 4732: 4577: 4539: 4538: 4529: 4523: 4522: 4509: 4508: 4496: 4432: 4407: 4406: 4397: 4391: 4390: 4377: 4376: 4364: 4300: 4211: 4191: 4171: 4162:Correspondence with nonlinear connections 4093: 4043: 4027: 4012: 3990: 3972: 3971: 3969: 3921: 3874: 3873: 3850: 3790: 3780: 3749: 3720: 3686: 3660: 3632: 3626: 3588: 3572: 3557: 3547: 3527: 3517: 3504: 3491: 3477: 3464: 3451: 3445: 3364: 3256: 3240: 3217: 3133: 3120: 3104: 3093: 3092: 3079: 3069: 3064: 3051: 3041: 3031: 3026: 3020: 3019: 3006: 2993: 2992: 2980: 2974: 2973: 2957: 2955: 2925: 2924: 2915: 2897: 2888: 2875: 2862: 2844: 2837: 2831: 2830: 2816: 2810: 2786: 2780: 2745: 2729: 2716: 2698: 2691: 2685: 2672: 2659: 2658: 2649: 2631: 2622: 2609: 2596: 2578: 2571: 2565: 2564: 2553: 2526: 2510: 2497: 2479: 2472: 2466: 2453: 2437: 2424: 2406: 2399: 2393: 2374: 2368: 2317: 2298: 2218: 2196: 2149: 2142: 2102: 2095: 2071: 2059: 2037: 2030: 1999: 1987: 1943: 1930: 1912: 1904: 1877: 1871: 1850: 1845: 1835: 1819: 1785: 1772: 1766: 1732: 1727: 1702: 1697: 1690: 1662: 1649: 1643: 1610: 1598: 1571: 1559: 1515: 1496: 1472: 1466: 1442: 1437: 1424: 1419: 1412: 1384: 1371: 1365: 1298: 1288: 1287: 1278: 1260: 1251: 1240: 1239: 1229: 1216: 1198: 1191: 1182: 1171: 1170: 1160: 1147: 1129: 1122: 1116: 1115: 1109: 1104: 1091: 1078: 1060: 1054: 1049: 1043: 1042: 1029: 1016: 1015: 1003: 997: 996: 980: 978: 923: 922: 895: 890: 868: 867: 865: 811: 777: 767: 736: 730: 673: 667: 666: 656: 643: 622: 594: 588: 587: 577: 564: 558: 545: 539: 516: 496: 476: 455: 446: 423: 399: 386: 377: 3193:The locally length minimizing curves of 707:on each associated coordinate system on 5183: 5099:Jacobi fields of sprays and semi-sprays 4696:Introducing the canonical vector field 4476: 4452: 4344: 4320: 4273: 4249: 4225: 2047:{\displaystyle \displaystyle g_{\xi }} 715:is a (full) spray, if and only if the 441:associated with the local coordinates 5214:Fundamentals of Differential Geometry 7: 5172:What is Kosambi-Cartan-Chern theory? 3343:,ξ) is simply the Riemannian metric 826:Semi-sprays in Lagrangian mechanics 5044: 5027: 4994: 4967: 4905: 4741: 3309:. In the Riemannian case one uses 2908: 2900: 2868: 2855: 2841: 2722: 2709: 2695: 2642: 2634: 2602: 2589: 2575: 2503: 2490: 2476: 2430: 2417: 2403: 2191:associated with the Lagrangian is 1936: 1923: 1909: 1607: 1508: 1500: 1271: 1263: 1222: 1209: 1195: 1153: 1140: 1126: 1071: 1063: 649: 645: 570: 566: 14: 5204:Lectures on Differential Geometry 5194:, Editura Academiei Române, 2007. 4716:of the semispray is known as the 2356:in the associated coordinates on 966:In the associated coordinates on 333:along the canonical vector field 223:is the canonical vector field on 5140:Jacobi equations of a semi-spray 5106: 4206:defines an Ehresmann-connection 411:{\displaystyle (x^{i},\xi ^{i})} 108:, and conversely, any semispray 5142:of the publicly available book 4489: 4485: 4357: 4353: 3744: 3681: 3536: 3486: 3414: 1758:associated with the Lagrangian. 801: 5159:Kosambi bi-derivative operator 5064: 5058: 5038: 5033: 5021: 5012: 4990: 4946: 4839: 4827: 4676: 4658: 4649: 4631: 4622: 4604: 4595: 4583: 4482: 4467: 4461: 4458: 4443: 4350: 4335: 4329: 4326: 4311: 4279: 4264: 4255: 4240: 4231: 4216: 4148:) and the corresponding flow Φ 4116: 4113: 4101: 4066: 4054: 4040: 4033: 4005: 3993: 3984: 3978: 3944: 3941: 3929: 3894: 3891: 3885: 3867: 3861: 3855: 3808: 3796: 3770: 3755: 3738: 3726: 3707: 3692: 3675: 3669: 3650: 3641: 3408: 3396: 3384: 3369: 3274: 3262: 3234: 3222: 3126: 3088: 3012: 2999: 2804: 2792: 2245: 2239: 2230: 2224: 2208: 2202: 2170: 2158: 2123: 2111: 2083:{\displaystyle \xi \in T_{x}M} 2011:{\displaystyle \xi \in T_{x}M} 1965: 1953: 1898: 1886: 1846: 1841: 1809: 1806: 1794: 1715: 1703: 1698: 1680: 1668: 1625: 1616: 1583:{\displaystyle \xi \in T_{x}M} 1537: 1525: 1490: 1478: 1420: 1402: 1390: 1035: 1022: 943: 940: 934: 916: 910: 904: 880: 874: 795: 783: 757: 742: 686: 674: 640: 628: 607: 595: 448: 405: 379: 16:Vector field on tangent bundle 1: 5169:'s methods, see the article, 4125:{\displaystyle \gamma :\to M} 3953:{\displaystyle \gamma :\to M} 2090:. Then the inverse matrix of 2021:The Lagrangian satisfies the 5149:dynamic covariant derivative 2772:with the spray coefficients 2275:, and there exists a unique 849:of some configuration space 418:be the local coordinates on 326:by a positive scalar λ>0. 5165:For a good introduction to 2054:is non-degenerate at every 1593:The corresponding one-form 5253: 5202:Sternberg, Shlomo (1964), 3186: 3180: 2025:if the fundamental tensor 80:Sprays arise naturally in 5192:Finsler-Lagrange Geometry 5144:Finsler-Lagrange Geometry 4140:of the Finsler manifold ( 2277:Hamiltonian vector field 5190:I. Bucataru, R. Miron, 4724:itself decomposes into 134:differentiable manifold 5082: 4976: 4918: 4857: 4761: 4712:. The vertical part ε= 4687: 4552: 4420: 4286: 4200: 4180: 4126: 4079: 3954: 3907: 3818: 3601: 3428: 3284: 3152: 2938: 2755: 2536: 2334: 2253: 2178: 2131: 2084: 2048: 2012: 1972: 1860: 1748: 1632: 1584: 1544: 1455: 1317: 956: 816: 698: 525: 505: 485: 465: 464:{\displaystyle (x^{i}} 435: 412: 329:The Lie-derivative of 5232:Differential geometry 5083: 4959: 4919: 4858: 4762: 4718:first spray invariant 4688: 4553: 4421: 4287: 4201: 4186:on a smooth manifold 4181: 4127: 4080: 3955: 3908: 3819: 3602: 3429: 3285: 3187:Further information: 3153: 2939: 2756: 2537: 2335: 2254: 2179: 2132: 2085: 2049: 2013: 1982:of the Lagrangian at 1973: 1861: 1749: 1633: 1585: 1545: 1456: 1318: 957: 817: 699: 526: 506: 486: 466: 436: 413: 261:is seen as a mapping 164:double tangent bundle 21:differential geometry 5212:Lang, Serge (1999), 4938: 4873: 4777: 4731: 4720:, and the semispray 4576: 4431: 4299: 4210: 4190: 4170: 4092: 3968: 3920: 3849: 3625: 3444: 3363: 3216: 2954: 2779: 2552: 2367: 2297: 2195: 2141: 2094: 2058: 2029: 1986: 1870: 1765: 1642: 1597: 1558: 1465: 1364: 977: 864: 729: 538: 515: 495: 475: 445: 422: 376: 344:The integral curves 104:induces a semispray 98:Lagrangian mechanics 5057: 5010: 4561:This connection on 4088:Therefore, a curve 3074: 3036: 1737: 1447: 1114: 1059: 900: 832:Lagrangian function 511:is a semi-spray on 368:(ξ) for any λ>0. 5118:. You can help by 5078: 5043: 4993: 4914: 4853: 4816: 4757: 4756: 4683: 4682: 4548: 4506: 4416: 4374: 4282: 4196: 4176: 4154:(ξ) is called the 4122: 4075: 3950: 3903: 3814: 3597: 3582: 3424: 3280: 3250: 3148: 3060: 3018: 2934: 2751: 2532: 2330: 2329: 2249: 2248: 2174: 2173: 2127: 2126: 2080: 2044: 2043: 2023:Legendre condition 2008: 1980:fundamental tensor 1968: 1951: 1856: 1761:The bilinear form 1744: 1723: 1628: 1580: 1552:conjugate momentum 1540: 1523: 1451: 1433: 1313: 1100: 1041: 952: 886: 812: 717:spray coefficients 694: 521: 501: 481: 461: 434:{\displaystyle TM} 431: 408: 124:Formal definitions 5216:, Springer-Verlag 5136: 5135: 5095:is a full spray. 4815: 4505: 4373: 4199:{\displaystyle M} 4179:{\displaystyle H} 4070: 4022: 3882: 3581: 3249: 3199:Finsler manifolds 3101: 2970: 2922: 2882: 2828: 2736: 2656: 2616: 2517: 2444: 1950: 1522: 1285: 1248: 1236: 1179: 1167: 1085: 993: 931: 663: 584: 524:{\displaystyle M} 504:{\displaystyle H} 484:{\displaystyle M} 213:tangent structure 5244: 5237:Finsler geometry 5217: 5207: 5195: 5188: 5131: 5128: 5110: 5103: 5087: 5085: 5084: 5079: 5068: 5067: 5056: 5051: 5041: 5020: 5019: 5009: 5001: 4989: 4988: 4975: 4970: 4955: 4954: 4949: 4923: 4921: 4920: 4915: 4889: 4888: 4883: 4882: 4862: 4860: 4859: 4854: 4849: 4848: 4825: 4824: 4817: 4808: 4799: 4798: 4793: 4792: 4766: 4764: 4763: 4758: 4692: 4690: 4689: 4684: 4557: 4555: 4554: 4549: 4544: 4543: 4534: 4533: 4528: 4527: 4514: 4513: 4507: 4498: 4425: 4423: 4422: 4417: 4412: 4411: 4402: 4401: 4396: 4395: 4382: 4381: 4375: 4366: 4291: 4289: 4288: 4283: 4205: 4203: 4202: 4197: 4185: 4183: 4182: 4177: 4131: 4129: 4128: 4123: 4084: 4082: 4081: 4076: 4071: 4069: 4049: 4048: 4047: 4028: 4023: 4018: 4017: 4016: 3991: 3977: 3976: 3959: 3957: 3956: 3951: 3912: 3910: 3909: 3904: 3884: 3883: 3875: 3823: 3821: 3820: 3815: 3795: 3794: 3785: 3784: 3754: 3753: 3725: 3724: 3691: 3690: 3668: 3667: 3640: 3639: 3606: 3604: 3603: 3598: 3593: 3592: 3583: 3574: 3562: 3561: 3552: 3551: 3532: 3531: 3522: 3521: 3512: 3511: 3496: 3495: 3482: 3481: 3472: 3471: 3456: 3455: 3433: 3431: 3430: 3425: 3307:Finsler function 3289: 3287: 3286: 3281: 3261: 3260: 3251: 3242: 3157: 3155: 3154: 3149: 3138: 3137: 3125: 3124: 3109: 3108: 3103: 3102: 3094: 3087: 3086: 3073: 3068: 3056: 3055: 3046: 3045: 3035: 3030: 3025: 3024: 3011: 3010: 2998: 2997: 2991: 2990: 2979: 2978: 2971: 2969: 2958: 2943: 2941: 2940: 2935: 2930: 2929: 2923: 2921: 2920: 2919: 2906: 2898: 2893: 2892: 2883: 2881: 2880: 2879: 2867: 2866: 2853: 2849: 2848: 2838: 2836: 2835: 2829: 2824: 2823: 2811: 2791: 2790: 2760: 2758: 2757: 2752: 2750: 2749: 2737: 2735: 2734: 2733: 2721: 2720: 2707: 2703: 2702: 2692: 2690: 2689: 2677: 2676: 2664: 2663: 2657: 2655: 2654: 2653: 2640: 2632: 2627: 2626: 2617: 2615: 2614: 2613: 2601: 2600: 2587: 2583: 2582: 2572: 2570: 2569: 2541: 2539: 2538: 2533: 2531: 2530: 2518: 2516: 2515: 2514: 2502: 2501: 2488: 2484: 2483: 2473: 2471: 2470: 2458: 2457: 2445: 2443: 2442: 2441: 2429: 2428: 2415: 2411: 2410: 2400: 2398: 2397: 2379: 2378: 2339: 2337: 2336: 2331: 2322: 2321: 2258: 2256: 2255: 2250: 2223: 2222: 2183: 2181: 2180: 2175: 2157: 2156: 2136: 2134: 2133: 2128: 2110: 2109: 2089: 2087: 2086: 2081: 2076: 2075: 2053: 2051: 2050: 2045: 2042: 2041: 2017: 2015: 2014: 2009: 2004: 2003: 1977: 1975: 1974: 1969: 1952: 1949: 1948: 1947: 1935: 1934: 1921: 1917: 1916: 1906: 1885: 1884: 1865: 1863: 1862: 1857: 1855: 1854: 1849: 1840: 1839: 1824: 1823: 1793: 1792: 1777: 1776: 1753: 1751: 1750: 1745: 1736: 1731: 1719: 1718: 1701: 1695: 1694: 1667: 1666: 1654: 1653: 1637: 1635: 1634: 1629: 1615: 1614: 1589: 1587: 1586: 1581: 1576: 1575: 1549: 1547: 1546: 1541: 1524: 1521: 1520: 1519: 1506: 1498: 1477: 1476: 1460: 1458: 1457: 1452: 1446: 1441: 1429: 1428: 1423: 1417: 1416: 1389: 1388: 1376: 1375: 1322: 1320: 1319: 1314: 1303: 1302: 1293: 1292: 1286: 1284: 1283: 1282: 1269: 1261: 1256: 1255: 1250: 1249: 1241: 1237: 1235: 1234: 1233: 1221: 1220: 1207: 1203: 1202: 1192: 1187: 1186: 1181: 1180: 1172: 1168: 1166: 1165: 1164: 1152: 1151: 1138: 1134: 1133: 1123: 1121: 1120: 1113: 1108: 1096: 1095: 1086: 1084: 1083: 1082: 1069: 1061: 1058: 1053: 1048: 1047: 1034: 1033: 1021: 1020: 1014: 1013: 1002: 1001: 994: 992: 981: 961: 959: 958: 953: 933: 932: 924: 899: 894: 873: 872: 821: 819: 818: 813: 782: 781: 772: 771: 741: 740: 711:. The semispray 703: 701: 700: 695: 690: 689: 672: 671: 664: 662: 661: 660: 644: 627: 626: 611: 610: 593: 592: 585: 583: 582: 581: 565: 563: 562: 550: 549: 530: 528: 527: 522: 510: 508: 507: 502: 490: 488: 487: 482: 470: 468: 467: 462: 460: 459: 440: 438: 437: 432: 417: 415: 414: 409: 404: 403: 391: 390: 86:Finsler geometry 5252: 5251: 5247: 5246: 5245: 5243: 5242: 5241: 5222: 5221: 5211: 5206:, Prentice-Hall 5201: 5198: 5189: 5185: 5181: 5132: 5126: 5123: 5116:needs expansion 5101: 5036: 5011: 4977: 4944: 4936: 4935: 4876: 4871: 4870: 4818: 4786: 4775: 4774: 4729: 4728: 4574: 4573: 4521: 4429: 4428: 4389: 4297: 4296: 4208: 4207: 4188: 4187: 4168: 4167: 4164: 4153: 4090: 4089: 4050: 4039: 4029: 4008: 3992: 3966: 3965: 3918: 3917: 3847: 3846: 3841: 3786: 3776: 3745: 3716: 3682: 3656: 3628: 3623: 3622: 3584: 3553: 3543: 3523: 3513: 3500: 3487: 3473: 3460: 3447: 3442: 3441: 3361: 3360: 3351: 3338: 3325: 3252: 3214: 3213: 3191: 3185: 3179: 3177:Geodesic spray 3129: 3116: 3091: 3075: 3047: 3037: 3002: 2972: 2962: 2952: 2951: 2911: 2907: 2899: 2884: 2871: 2858: 2854: 2840: 2839: 2812: 2782: 2777: 2776: 2741: 2725: 2712: 2708: 2694: 2693: 2681: 2668: 2645: 2641: 2633: 2618: 2605: 2592: 2588: 2574: 2573: 2550: 2549: 2522: 2506: 2493: 2489: 2475: 2474: 2462: 2449: 2433: 2420: 2416: 2402: 2401: 2389: 2370: 2365: 2364: 2313: 2295: 2294: 2273:symplectic form 2214: 2193: 2192: 2145: 2139: 2138: 2098: 2092: 2091: 2067: 2056: 2055: 2033: 2027: 2026: 1995: 1984: 1983: 1939: 1926: 1922: 1908: 1907: 1873: 1868: 1867: 1844: 1831: 1815: 1781: 1768: 1763: 1762: 1696: 1686: 1658: 1645: 1640: 1639: 1606: 1595: 1594: 1567: 1556: 1555: 1511: 1507: 1499: 1468: 1463: 1462: 1418: 1408: 1380: 1367: 1362: 1361: 1351: 1339: 1294: 1274: 1270: 1262: 1238: 1225: 1212: 1208: 1194: 1193: 1169: 1156: 1143: 1139: 1125: 1124: 1087: 1074: 1070: 1062: 1025: 995: 985: 975: 974: 862: 861: 828: 773: 763: 732: 727: 726: 665: 652: 648: 618: 586: 573: 569: 554: 541: 536: 535: 513: 512: 493: 492: 473: 472: 451: 443: 442: 420: 419: 395: 382: 374: 373: 367: 363: 351: 309: 305: 298: 294: 196: 190: 186: 145: 126: 94:integral curves 90:geodesic sprays 68: 64: 61:obey the rule Φ 56: 41:that encodes a 17: 12: 11: 5: 5250: 5248: 5240: 5239: 5234: 5224: 5223: 5220: 5219: 5209: 5197: 5196: 5182: 5180: 5177: 5134: 5133: 5113: 5111: 5100: 5097: 5089: 5088: 5077: 5074: 5071: 5066: 5063: 5060: 5055: 5050: 5046: 5040: 5035: 5032: 5029: 5026: 5023: 5018: 5014: 5008: 5005: 5000: 4996: 4992: 4987: 4984: 4980: 4974: 4969: 4966: 4962: 4958: 4953: 4948: 4943: 4925: 4924: 4913: 4910: 4907: 4904: 4901: 4898: 4895: 4892: 4887: 4881: 4864: 4863: 4852: 4847: 4844: 4841: 4838: 4835: 4832: 4829: 4823: 4814: 4811: 4805: 4802: 4797: 4791: 4785: 4782: 4768: 4767: 4755: 4752: 4749: 4746: 4743: 4740: 4737: 4694: 4693: 4681: 4678: 4675: 4672: 4669: 4666: 4663: 4660: 4657: 4654: 4651: 4648: 4645: 4642: 4639: 4636: 4633: 4630: 4627: 4624: 4621: 4618: 4615: 4612: 4609: 4606: 4603: 4600: 4597: 4594: 4591: 4588: 4585: 4582: 4559: 4558: 4547: 4542: 4537: 4532: 4526: 4520: 4517: 4512: 4504: 4501: 4495: 4492: 4488: 4484: 4481: 4478: 4475: 4472: 4469: 4466: 4463: 4460: 4457: 4454: 4451: 4448: 4445: 4442: 4439: 4436: 4426: 4415: 4410: 4405: 4400: 4394: 4388: 4385: 4380: 4372: 4369: 4363: 4360: 4356: 4352: 4349: 4346: 4343: 4340: 4337: 4334: 4331: 4328: 4325: 4322: 4319: 4316: 4313: 4310: 4307: 4304: 4281: 4278: 4275: 4272: 4269: 4266: 4263: 4260: 4257: 4254: 4251: 4248: 4245: 4242: 4239: 4236: 4233: 4230: 4227: 4224: 4221: 4218: 4215: 4195: 4175: 4163: 4160: 4149: 4138:geodesic spray 4136:is called the 4121: 4118: 4115: 4112: 4109: 4106: 4103: 4100: 4097: 4086: 4085: 4074: 4068: 4065: 4062: 4059: 4056: 4053: 4046: 4042: 4038: 4035: 4032: 4026: 4021: 4015: 4011: 4007: 4004: 4001: 3998: 3995: 3989: 3986: 3983: 3980: 3975: 3962: 3961: 3949: 3946: 3943: 3940: 3937: 3934: 3931: 3928: 3925: 3916:For any curve 3914: 3902: 3899: 3896: 3893: 3890: 3887: 3881: 3878: 3872: 3869: 3866: 3863: 3860: 3857: 3854: 3843: 3839: 3825: 3824: 3813: 3810: 3807: 3804: 3801: 3798: 3793: 3789: 3783: 3779: 3775: 3772: 3769: 3766: 3763: 3760: 3757: 3752: 3748: 3743: 3740: 3737: 3734: 3731: 3728: 3723: 3719: 3715: 3712: 3709: 3706: 3703: 3700: 3697: 3694: 3689: 3685: 3680: 3677: 3674: 3671: 3666: 3663: 3659: 3655: 3652: 3649: 3646: 3643: 3638: 3635: 3631: 3608: 3607: 3596: 3591: 3587: 3580: 3577: 3571: 3568: 3565: 3560: 3556: 3550: 3546: 3542: 3539: 3535: 3530: 3526: 3520: 3516: 3510: 3507: 3503: 3499: 3494: 3490: 3485: 3480: 3476: 3470: 3467: 3463: 3459: 3454: 3450: 3435: 3434: 3423: 3420: 3417: 3413: 3410: 3407: 3404: 3401: 3398: 3395: 3392: 3389: 3386: 3383: 3380: 3377: 3374: 3371: 3368: 3347: 3334: 3321: 3291: 3290: 3279: 3276: 3273: 3270: 3267: 3264: 3259: 3255: 3248: 3245: 3239: 3236: 3233: 3230: 3227: 3224: 3221: 3183:Geodesic spray 3181:Main article: 3178: 3175: 3159: 3158: 3147: 3144: 3141: 3136: 3132: 3128: 3123: 3119: 3115: 3112: 3107: 3100: 3097: 3090: 3085: 3082: 3078: 3072: 3067: 3063: 3059: 3054: 3050: 3044: 3040: 3034: 3029: 3023: 3017: 3014: 3009: 3005: 3001: 2996: 2989: 2986: 2983: 2977: 2968: 2965: 2961: 2945: 2944: 2933: 2928: 2918: 2914: 2910: 2905: 2902: 2896: 2891: 2887: 2878: 2874: 2870: 2865: 2861: 2857: 2852: 2847: 2843: 2834: 2827: 2822: 2819: 2815: 2809: 2806: 2803: 2800: 2797: 2794: 2789: 2785: 2762: 2761: 2748: 2744: 2740: 2732: 2728: 2724: 2719: 2715: 2711: 2706: 2701: 2697: 2688: 2684: 2680: 2675: 2671: 2667: 2662: 2652: 2648: 2644: 2639: 2636: 2630: 2625: 2621: 2612: 2608: 2604: 2599: 2595: 2591: 2586: 2581: 2577: 2568: 2563: 2560: 2557: 2543: 2542: 2529: 2525: 2521: 2513: 2509: 2505: 2500: 2496: 2492: 2487: 2482: 2478: 2469: 2465: 2461: 2456: 2452: 2448: 2440: 2436: 2432: 2427: 2423: 2419: 2414: 2409: 2405: 2396: 2392: 2388: 2385: 2382: 2377: 2373: 2342: 2341: 2328: 2325: 2320: 2316: 2312: 2309: 2306: 2303: 2261: 2260: 2247: 2244: 2241: 2238: 2235: 2232: 2229: 2226: 2221: 2217: 2213: 2210: 2207: 2204: 2201: 2185: 2172: 2169: 2166: 2163: 2160: 2155: 2152: 2148: 2137:is denoted by 2125: 2122: 2119: 2116: 2113: 2108: 2105: 2101: 2079: 2074: 2070: 2066: 2063: 2040: 2036: 2019: 2007: 2002: 1998: 1994: 1991: 1967: 1964: 1961: 1958: 1955: 1946: 1942: 1938: 1933: 1929: 1925: 1920: 1915: 1911: 1903: 1900: 1897: 1894: 1891: 1888: 1883: 1880: 1876: 1853: 1848: 1843: 1838: 1834: 1830: 1827: 1822: 1818: 1814: 1811: 1808: 1805: 1802: 1799: 1796: 1791: 1788: 1784: 1780: 1775: 1771: 1759: 1743: 1740: 1735: 1730: 1726: 1722: 1717: 1714: 1711: 1708: 1705: 1700: 1693: 1689: 1685: 1682: 1679: 1676: 1673: 1670: 1665: 1661: 1657: 1652: 1648: 1627: 1624: 1621: 1618: 1613: 1609: 1605: 1602: 1591: 1579: 1574: 1570: 1566: 1563: 1539: 1536: 1533: 1530: 1527: 1518: 1514: 1510: 1505: 1502: 1495: 1492: 1489: 1486: 1483: 1480: 1475: 1471: 1450: 1445: 1440: 1436: 1432: 1427: 1422: 1415: 1411: 1407: 1404: 1401: 1398: 1395: 1392: 1387: 1383: 1379: 1374: 1370: 1349: 1335: 1324: 1323: 1312: 1309: 1306: 1301: 1297: 1291: 1281: 1277: 1273: 1268: 1265: 1259: 1254: 1247: 1244: 1232: 1228: 1224: 1219: 1215: 1211: 1206: 1201: 1197: 1190: 1185: 1178: 1175: 1163: 1159: 1155: 1150: 1146: 1142: 1137: 1132: 1128: 1119: 1112: 1107: 1103: 1099: 1094: 1090: 1081: 1077: 1073: 1068: 1065: 1057: 1052: 1046: 1040: 1037: 1032: 1028: 1024: 1019: 1012: 1009: 1006: 1000: 991: 988: 984: 964: 963: 951: 948: 945: 942: 939: 936: 930: 927: 921: 918: 915: 912: 909: 906: 903: 898: 893: 889: 885: 882: 879: 876: 871: 847:tangent bundle 827: 824: 823: 822: 810: 807: 804: 800: 797: 794: 791: 788: 785: 780: 776: 770: 766: 762: 759: 756: 753: 750: 747: 744: 739: 735: 705: 704: 693: 688: 685: 682: 679: 676: 670: 659: 655: 651: 647: 642: 639: 636: 633: 630: 625: 621: 617: 614: 609: 606: 603: 600: 597: 591: 580: 576: 572: 568: 561: 557: 553: 548: 544: 520: 500: 480: 458: 454: 450: 430: 427: 407: 402: 398: 394: 389: 385: 381: 370: 369: 365: 361: 349: 342: 327: 307: 303: 296: 292: 271: 270: 255:canonical flip 228: 198: 194: 188: 182: 141: 125: 122: 66: 62: 54: 36:tangent bundle 15: 13: 10: 9: 6: 4: 3: 2: 5249: 5238: 5235: 5233: 5230: 5229: 5227: 5215: 5210: 5205: 5200: 5199: 5193: 5187: 5184: 5178: 5176: 5174: 5173: 5168: 5163: 5161: 5160: 5155: 5154:another paper 5151: 5150: 5145: 5141: 5130: 5127:February 2013 5121: 5117: 5114:This section 5112: 5109: 5105: 5104: 5098: 5096: 5094: 5075: 5072: 5069: 5061: 5053: 5048: 5030: 5024: 5016: 5006: 5003: 4998: 4985: 4982: 4978: 4972: 4964: 4960: 4956: 4951: 4941: 4934: 4933: 4932: 4930: 4911: 4908: 4902: 4899: 4896: 4893: 4890: 4885: 4869: 4868: 4867: 4850: 4845: 4842: 4836: 4833: 4830: 4812: 4809: 4803: 4800: 4795: 4783: 4780: 4773: 4772: 4771: 4753: 4750: 4747: 4744: 4738: 4735: 4727: 4726: 4725: 4723: 4719: 4715: 4711: 4707: 4703: 4699: 4679: 4673: 4670: 4667: 4664: 4661: 4655: 4652: 4646: 4643: 4640: 4637: 4634: 4628: 4625: 4619: 4616: 4613: 4610: 4607: 4601: 4598: 4592: 4589: 4586: 4580: 4572: 4571: 4570: 4568: 4564: 4545: 4535: 4530: 4518: 4515: 4502: 4499: 4493: 4490: 4486: 4479: 4473: 4470: 4464: 4455: 4449: 4446: 4440: 4437: 4434: 4427: 4413: 4403: 4398: 4386: 4383: 4370: 4367: 4361: 4358: 4354: 4347: 4341: 4338: 4332: 4323: 4317: 4314: 4308: 4305: 4302: 4295: 4294: 4293: 4276: 4270: 4267: 4261: 4258: 4252: 4246: 4243: 4237: 4234: 4228: 4222: 4219: 4213: 4193: 4173: 4166:A semi-spray 4161: 4159: 4157: 4156:geodesic flow 4152: 4147: 4143: 4139: 4135: 4119: 4110: 4107: 4104: 4098: 4095: 4072: 4063: 4060: 4057: 4051: 4044: 4036: 4030: 4024: 4019: 4013: 4009: 4002: 3999: 3996: 3987: 3981: 3964: 3963: 3947: 3938: 3935: 3932: 3926: 3923: 3915: 3900: 3897: 3888: 3879: 3876: 3870: 3864: 3858: 3852: 3844: 3838: 3834: 3833: 3832: 3830: 3811: 3805: 3802: 3799: 3791: 3787: 3781: 3777: 3773: 3767: 3764: 3761: 3758: 3750: 3746: 3741: 3735: 3732: 3729: 3721: 3717: 3713: 3710: 3704: 3701: 3698: 3695: 3687: 3683: 3678: 3672: 3664: 3661: 3657: 3653: 3647: 3644: 3636: 3633: 3629: 3621: 3620: 3619: 3617: 3613: 3594: 3589: 3585: 3578: 3575: 3569: 3566: 3563: 3558: 3554: 3548: 3544: 3540: 3537: 3533: 3528: 3524: 3518: 3514: 3508: 3505: 3501: 3497: 3492: 3488: 3483: 3478: 3474: 3468: 3465: 3461: 3457: 3452: 3448: 3440: 3439: 3438: 3421: 3418: 3415: 3411: 3405: 3402: 3399: 3393: 3390: 3387: 3381: 3378: 3375: 3372: 3366: 3359: 3358: 3357: 3355: 3350: 3346: 3342: 3337: 3333: 3329: 3324: 3320: 3316: 3312: 3308: 3304: 3300: 3296: 3277: 3271: 3268: 3265: 3257: 3253: 3246: 3243: 3237: 3231: 3228: 3225: 3219: 3212: 3211: 3210: 3208: 3204: 3200: 3196: 3190: 3189:Geodesic flow 3184: 3176: 3174: 3172: 3168: 3164: 3161:and we see γ→ 3145: 3142: 3139: 3134: 3130: 3121: 3117: 3113: 3110: 3105: 3098: 3095: 3083: 3080: 3076: 3070: 3065: 3061: 3057: 3052: 3048: 3042: 3038: 3032: 3027: 3015: 3007: 3003: 2987: 2984: 2981: 2966: 2963: 2959: 2950: 2949: 2948: 2931: 2916: 2912: 2903: 2894: 2889: 2885: 2876: 2872: 2863: 2859: 2850: 2845: 2825: 2820: 2817: 2813: 2807: 2801: 2798: 2795: 2787: 2783: 2775: 2774: 2773: 2771: 2767: 2746: 2742: 2738: 2730: 2726: 2717: 2713: 2704: 2699: 2686: 2682: 2678: 2673: 2669: 2665: 2650: 2646: 2637: 2628: 2623: 2619: 2610: 2606: 2597: 2593: 2584: 2579: 2561: 2558: 2555: 2548: 2547: 2546: 2527: 2523: 2519: 2511: 2507: 2498: 2494: 2485: 2480: 2467: 2463: 2459: 2454: 2450: 2446: 2438: 2434: 2425: 2421: 2412: 2407: 2394: 2390: 2386: 2383: 2380: 2375: 2371: 2363: 2362: 2361: 2359: 2355: 2351: 2347: 2326: 2323: 2318: 2314: 2310: 2307: 2304: 2301: 2293: 2292: 2291: 2289: 2285: 2281: 2278: 2274: 2270: 2266: 2242: 2236: 2233: 2227: 2219: 2215: 2211: 2205: 2199: 2190: 2186: 2167: 2164: 2161: 2153: 2150: 2146: 2120: 2117: 2114: 2106: 2103: 2099: 2077: 2072: 2068: 2064: 2061: 2038: 2034: 2024: 2020: 2005: 2000: 1996: 1992: 1989: 1981: 1962: 1959: 1956: 1944: 1940: 1931: 1927: 1918: 1913: 1901: 1895: 1892: 1889: 1881: 1878: 1874: 1851: 1836: 1832: 1828: 1825: 1820: 1816: 1812: 1803: 1800: 1797: 1789: 1786: 1782: 1778: 1773: 1769: 1760: 1757: 1741: 1738: 1733: 1728: 1724: 1720: 1712: 1709: 1706: 1691: 1687: 1683: 1677: 1674: 1671: 1663: 1659: 1655: 1650: 1646: 1622: 1619: 1611: 1603: 1600: 1592: 1577: 1572: 1568: 1564: 1561: 1553: 1534: 1531: 1528: 1516: 1512: 1503: 1493: 1487: 1484: 1481: 1473: 1469: 1448: 1443: 1438: 1434: 1430: 1425: 1413: 1409: 1405: 1399: 1396: 1393: 1385: 1381: 1377: 1372: 1368: 1360:The covector 1359: 1358: 1357: 1355: 1347: 1343: 1338: 1333: 1329: 1310: 1307: 1304: 1299: 1295: 1279: 1275: 1266: 1257: 1252: 1245: 1242: 1230: 1226: 1217: 1213: 1204: 1199: 1188: 1183: 1176: 1173: 1161: 1157: 1148: 1144: 1135: 1130: 1110: 1105: 1101: 1097: 1092: 1088: 1079: 1075: 1066: 1055: 1050: 1038: 1030: 1026: 1010: 1007: 1004: 989: 986: 982: 973: 972: 971: 969: 949: 946: 937: 928: 925: 919: 913: 907: 901: 896: 891: 887: 883: 877: 860: 859: 858: 856: 852: 848: 844: 840: 836: 833: 825: 808: 805: 802: 798: 792: 789: 786: 778: 774: 768: 764: 760: 754: 751: 748: 745: 737: 733: 725: 724: 723: 721: 718: 714: 710: 691: 683: 680: 677: 657: 653: 637: 634: 631: 623: 619: 615: 612: 604: 601: 598: 578: 574: 559: 555: 551: 546: 542: 534: 533: 532: 518: 498: 478: 456: 452: 428: 425: 400: 396: 392: 387: 383: 359: 355: 347: 343: 340: 336: 332: 328: 325: 321: 317: 313: 302: 291: 288: 287: 286: 284: 280: 276: 268: 264: 260: 256: 252: 248: 244: 240: 236: 232: 229: 226: 222: 218: 214: 210: 206: 202: 199: 193: 185: 180: 179: 178: 176: 172: 168: 165: 161: 157: 153: 149: 144: 139: 135: 131: 123: 121: 119: 115: 111: 107: 103: 99: 95: 91: 87: 83: 78: 76: 72: 60: 52: 48: 44: 40: 37: 33: 30: 26: 22: 5213: 5203: 5191: 5186: 5170: 5164: 5157: 5147: 5143: 5139: 5137: 5124: 5120:adding to it 5115: 5092: 5090: 4928: 4926: 4865: 4769: 4721: 4717: 4713: 4709: 4705: 4701: 4697: 4695: 4566: 4562: 4560: 4165: 4155: 4150: 4145: 4141: 4137: 4133: 4087: 3836: 3828: 3826: 3615: 3611: 3609: 3436: 3353: 3348: 3344: 3340: 3335: 3331: 3327: 3322: 3318: 3314: 3310: 3302: 3298: 3294: 3292: 3206: 3192: 3170: 3166: 3162: 3160: 2946: 2769: 2765: 2763: 2544: 2357: 2353: 2349: 2345: 2343: 2287: 2283: 2279: 2268: 2264: 2262: 2188: 2022: 1979: 1756:Hilbert-form 1755: 1551: 1353: 1345: 1341: 1336: 1331: 1327: 1325: 967: 965: 854: 850: 842: 838: 834: 829: 719: 716: 712: 708: 706: 371: 357: 353: 345: 338: 334: 330: 323: 319: 315: 311: 300: 289: 283:(full) spray 282: 278: 274: 273:A semispray 272: 266: 262: 258: 250: 246: 242: 238: 234: 230: 224: 220: 216: 208: 204: 200: 191: 183: 174: 170: 166: 158:(that is, a 155: 151: 147: 142: 137: 129: 127: 117: 113: 109: 105: 101: 79: 74: 73:is called a 70: 58: 50: 46: 38: 31: 29:vector field 24: 18: 3201:are called 337:satisfies = 43:quasilinear 5226:Categories 5179:References 3195:Riemannian 2290:such that 306:), where λ 171:semi-spray 82:Riemannian 75:semi-spray 5062:ξ 5045:Φ 5028:Θ 5025:τ 5017:∗ 5004:− 4995:Φ 4983:− 4968:∞ 4965:− 4961:∫ 4952:ξ 4942:ϵ 4906:Θ 4903:τ 4897:ϵ 4891:ϵ 4843:− 4781:τ 4751:ϵ 4742:Θ 4653:− 4626:− 4477:∖ 4462:→ 4453:∖ 4387:− 4345:∖ 4330:→ 4321:∖ 4274:∖ 4259:⊕ 4250:∖ 4226:∖ 4117:→ 4096:γ 4061:− 4037:γ 4031:ℓ 4010:λ 4000:− 3982:γ 3945:→ 3924:γ 3901:λ 3880:˙ 3877:γ 3859:γ 3806:ξ 3778:λ 3768:ξ 3765:λ 3736:ξ 3718:α 3714:λ 3705:ξ 3702:λ 3684:α 3673:ξ 3648:ξ 3645:λ 3564:− 3555:ξ 3545:α 3525:ξ 3515:ξ 3475:ξ 3449:α 3416:λ 3406:ξ 3391:λ 3382:ξ 3379:λ 3272:ξ 3232:ξ 3203:geodesics 3099:¨ 3096:γ 3062:∫ 3058:− 3039:α 3004:γ 2909:∂ 2901:∂ 2895:− 2886:ξ 2869:∂ 2860:ξ 2856:∂ 2842:∂ 2802:ξ 2743:ξ 2723:∂ 2714:ξ 2710:∂ 2696:∂ 2683:ξ 2643:∂ 2635:∂ 2629:− 2620:ξ 2607:ξ 2603:∂ 2590:∂ 2576:∂ 2524:ξ 2504:∂ 2495:ξ 2491:∂ 2477:∂ 2460:− 2431:∂ 2422:ξ 2418:∂ 2404:∂ 2384:α 2372:ι 2327:α 2315:ι 2311:− 2243:ξ 2234:− 2228:ξ 2220:ξ 2216:α 2206:ξ 2168:ξ 2121:ξ 2065:∈ 2062:ξ 2039:ξ 1993:∈ 1990:ξ 1963:ξ 1941:ξ 1937:∂ 1928:ξ 1924:∂ 1910:∂ 1896:ξ 1826:⊗ 1804:ξ 1774:ξ 1734:∗ 1729:ξ 1721:∈ 1713:ξ 1678:ξ 1660:α 1651:ξ 1647:α 1608:Ω 1604:∈ 1601:α 1565:∈ 1562:ξ 1535:ξ 1513:ξ 1509:∂ 1501:∂ 1488:ξ 1470:α 1444:∗ 1431:∈ 1400:ξ 1382:α 1373:ξ 1369:α 1344:around γ( 1272:∂ 1264:∂ 1258:− 1246:˙ 1243:γ 1227:ξ 1223:∂ 1210:∂ 1196:∂ 1177:¨ 1174:γ 1158:ξ 1154:∂ 1145:ξ 1141:∂ 1127:∂ 1102:∫ 1098:− 1076:ξ 1072:∂ 1064:∂ 1027:γ 929:˙ 926:γ 908:γ 888:∫ 878:γ 803:λ 793:ξ 765:λ 755:ξ 752:λ 684:ξ 654:ξ 650:∂ 646:∂ 638:ξ 613:− 605:ξ 571:∂ 567:∂ 556:ξ 547:ξ 397:ξ 360:satisfy Φ 722:satisfy 253:is the 241:, where 207:, where 5167:Kosambi 3305:is the 2360:. Then 2271:) is a 1978:is the 1754:is the 1550:is the 845:on the 364:(λξ)=λΦ 211:is the 169:) is a 162:of the 160:section 88:as the 34:on the 3835:Since 3317:,ξ) = 3293:where 2189:Energy 1326:where 356:\0 of 92:whose 65:(λξ)=Φ 5152:. In 2344:Let ( 1866:with 1638:with 1461:with 1348:) = γ 471:) on 281:is a 136:and ( 132:be a 27:is a 25:spray 3419:> 3197:and 2545:and 2267:α∈Ω( 2187:The 806:> 372:Let 352:(ξ)∈ 257:and 219:and 197:= ξ. 128:Let 84:and 57:(ξ)∈ 23:, a 5122:. 4700:on 3209:by 2282:on 1554:of 316:TTM 312:TTM 295:= λ 277:on 267:TTM 251:TTM 247:TTM 227:\0. 215:on 173:on 167:TTM 154:on 19:In 5228:: 5175:. 5162:. 4714:vH 4708:=Θ 4706:hH 4702:TM 4563:TM 4158:. 3349:ij 3336:ij 3323:ij 3299:TM 3207:TM 3167:TM 2358:TM 2284:TM 2269:TM 1340::→ 1330::→ 968:TM 884::= 839:TM 809:0. 709:TM 354:TM 348:→Φ 324:TM 320:TM 299:(λ 293:λξ 263:TM 225:TM 217:TM 201:JH 184:TM 181:(π 156:TM 143:TM 140:,π 138:TM 77:. 59:TM 53:→Φ 39:TM 5218:. 5208:. 5129:) 5125:( 5093:H 5076:. 5073:s 5070:d 5065:) 5059:( 5054:s 5049:V 5039:| 5034:) 5031:V 5022:( 5013:) 5007:s 4999:V 4991:( 4986:s 4979:e 4973:0 4957:= 4947:| 4929:H 4912:. 4909:V 4900:= 4894:+ 4886:V 4880:L 4851:J 4846:H 4840:] 4837:H 4834:, 4831:V 4828:[ 4822:L 4813:2 4810:1 4804:= 4801:v 4796:V 4790:L 4784:= 4754:. 4748:+ 4745:V 4739:= 4736:H 4722:H 4710:V 4698:V 4680:. 4677:] 4674:Y 4671:J 4668:, 4665:X 4662:h 4659:[ 4656:v 4650:] 4647:Y 4644:h 4641:, 4638:X 4635:J 4632:[ 4629:v 4623:] 4620:Y 4617:h 4614:, 4611:X 4608:h 4605:[ 4602:J 4599:= 4596:) 4593:Y 4590:, 4587:X 4584:( 4581:T 4567:T 4546:. 4541:) 4536:J 4531:H 4525:L 4519:+ 4516:I 4511:( 4503:2 4500:1 4494:= 4491:v 4487:; 4483:) 4480:0 4474:M 4471:T 4468:( 4465:T 4459:) 4456:0 4450:M 4447:T 4444:( 4441:T 4438:: 4435:v 4414:, 4409:) 4404:J 4399:H 4393:L 4384:I 4379:( 4371:2 4368:1 4362:= 4359:h 4355:; 4351:) 4348:0 4342:M 4339:T 4336:( 4333:T 4327:) 4324:0 4318:M 4315:T 4312:( 4309:T 4306:: 4303:h 4280:) 4277:0 4271:M 4268:T 4265:( 4262:V 4256:) 4253:0 4247:M 4244:T 4241:( 4238:H 4235:= 4232:) 4229:0 4223:M 4220:T 4217:( 4214:T 4194:M 4174:H 4151:H 4146:F 4144:, 4142:M 4134:H 4120:M 4114:] 4111:b 4108:, 4105:a 4102:[ 4099:: 4073:. 4067:) 4064:a 4058:b 4055:( 4052:2 4045:2 4041:) 4034:( 4025:= 4020:2 4014:2 4006:) 4003:a 3997:b 3994:( 3988:= 3985:) 3979:( 3974:S 3948:M 3942:] 3939:b 3936:, 3933:a 3930:[ 3927:: 3898:= 3895:) 3892:) 3889:t 3886:( 3871:, 3868:) 3865:t 3862:( 3856:( 3853:F 3840:ξ 3837:g 3829:H 3812:, 3809:) 3803:, 3800:x 3797:( 3792:i 3788:G 3782:2 3774:= 3771:) 3762:, 3759:x 3756:( 3751:i 3747:G 3742:, 3739:) 3733:, 3730:x 3727:( 3722:i 3711:= 3708:) 3699:, 3696:x 3693:( 3688:i 3679:, 3676:) 3670:( 3665:j 3662:i 3658:g 3654:= 3651:) 3642:( 3637:j 3634:i 3630:g 3616:L 3614:, 3612:M 3595:. 3590:2 3586:F 3579:2 3576:1 3570:= 3567:L 3559:i 3549:i 3541:= 3538:E 3534:, 3529:j 3519:i 3509:j 3506:i 3502:g 3498:= 3493:2 3489:F 3484:, 3479:i 3469:j 3466:i 3462:g 3458:= 3453:i 3422:0 3412:, 3409:) 3403:, 3400:x 3397:( 3394:F 3388:= 3385:) 3376:, 3373:x 3370:( 3367:F 3354:x 3352:( 3345:g 3341:x 3339:( 3332:g 3328:x 3326:( 3319:g 3315:x 3313:( 3311:F 3303:R 3301:→ 3297:: 3295:F 3278:, 3275:) 3269:, 3266:x 3263:( 3258:2 3254:F 3247:2 3244:1 3238:= 3235:) 3229:, 3226:x 3223:( 3220:L 3171:H 3163:M 3146:, 3143:t 3140:d 3135:i 3131:X 3127:) 3122:k 3118:G 3114:2 3111:+ 3106:k 3089:( 3084:k 3081:i 3077:g 3071:b 3066:a 3053:i 3049:X 3043:i 3033:b 3028:a 3022:| 3016:= 3013:) 3008:s 3000:( 2995:S 2988:0 2985:= 2982:s 2976:| 2967:s 2964:d 2960:d 2932:. 2927:) 2917:i 2913:x 2904:L 2890:j 2877:j 2873:x 2864:i 2851:L 2846:2 2833:( 2826:2 2821:i 2818:k 2814:g 2808:= 2805:) 2799:, 2796:x 2793:( 2788:k 2784:G 2770:M 2766:H 2747:i 2739:d 2731:j 2727:x 2718:i 2705:L 2700:2 2687:j 2679:+ 2674:i 2670:x 2666:d 2661:) 2651:i 2647:x 2638:L 2624:j 2611:j 2598:i 2594:x 2585:L 2580:2 2567:( 2562:= 2559:E 2556:d 2528:j 2520:d 2512:j 2508:x 2499:i 2486:L 2481:2 2468:i 2464:X 2455:j 2451:x 2447:d 2439:j 2435:x 2426:i 2413:L 2408:2 2395:i 2391:Y 2387:= 2381:d 2376:H 2354:H 2350:Y 2348:, 2346:X 2340:. 2324:d 2319:H 2308:= 2305:E 2302:d 2288:E 2280:H 2265:d 2259:. 2246:) 2240:( 2237:L 2231:) 2225:( 2212:= 2209:) 2203:( 2200:E 2184:. 2171:) 2165:, 2162:x 2159:( 2154:j 2151:i 2147:g 2124:) 2118:, 2115:x 2112:( 2107:j 2104:i 2100:g 2078:M 2073:x 2069:T 2035:g 2018:. 2006:M 2001:x 1997:T 1966:) 1960:, 1957:x 1954:( 1945:j 1932:i 1919:L 1914:2 1902:= 1899:) 1893:, 1890:x 1887:( 1882:j 1879:i 1875:g 1852:x 1847:| 1842:) 1837:j 1833:x 1829:d 1821:i 1817:x 1813:d 1810:( 1807:) 1801:, 1798:x 1795:( 1790:j 1787:i 1783:g 1779:= 1770:g 1742:M 1739:T 1725:T 1716:) 1710:, 1707:x 1704:( 1699:| 1692:i 1688:x 1684:d 1681:) 1675:, 1672:x 1669:( 1664:i 1656:= 1626:) 1623:M 1620:T 1617:( 1612:1 1590:. 1578:M 1573:x 1569:T 1538:) 1532:, 1529:x 1526:( 1517:i 1504:L 1494:= 1491:) 1485:, 1482:x 1479:( 1474:i 1449:M 1439:x 1435:T 1426:x 1421:| 1414:i 1410:x 1406:d 1403:) 1397:, 1394:x 1391:( 1386:i 1378:= 1354:t 1352:( 1350:0 1346:t 1342:M 1337:s 1332:R 1328:X 1311:, 1308:t 1305:d 1300:i 1296:X 1290:) 1280:i 1276:x 1267:L 1253:j 1231:i 1218:j 1214:x 1205:L 1200:2 1189:+ 1184:j 1162:i 1149:j 1136:L 1131:2 1118:( 1111:b 1106:a 1093:i 1089:X 1080:i 1067:L 1056:b 1051:a 1045:| 1039:= 1036:) 1031:s 1023:( 1018:S 1011:0 1008:= 1005:s 999:| 990:s 987:d 983:d 962:. 950:t 947:d 944:) 941:) 938:t 935:( 920:, 917:) 914:t 911:( 905:( 902:L 897:b 892:a 881:) 875:( 870:S 855:M 851:M 843:R 841:→ 837:: 835:L 799:, 796:) 790:, 787:x 784:( 779:i 775:G 769:2 761:= 758:) 749:, 746:x 743:( 738:i 734:G 720:G 713:H 692:. 687:) 681:, 678:x 675:( 669:| 658:i 641:) 635:, 632:x 629:( 624:i 620:G 616:2 608:) 602:, 599:x 596:( 590:| 579:i 575:x 560:i 552:= 543:H 519:M 499:H 479:M 457:i 453:x 449:( 429:M 426:T 406:) 401:i 393:, 388:i 384:x 380:( 366:H 362:H 358:H 350:H 346:t 341:. 339:H 335:V 331:H 322:→ 314:→ 310:: 308:* 304:ξ 301:H 297:* 290:H 279:M 275:H 269:. 265:→ 259:H 249:→ 245:: 243:j 239:H 237:= 235:H 233:∘ 231:j 221:V 209:J 205:V 203:= 195:ξ 192:H 189:* 187:) 175:M 152:H 148:M 146:, 130:M 118:H 114:M 110:H 106:H 102:M 71:H 67:H 63:H 55:H 51:t 47:M 32:H

Index

differential geometry
vector field
tangent bundle
quasilinear
Riemannian
Finsler geometry
geodesic sprays
integral curves
Lagrangian mechanics
differentiable manifold
section
double tangent bundle
tangent structure
canonical flip
Lagrangian function
tangent bundle
symplectic form
Hamiltonian vector field
Geodesic spray
Geodesic flow
Riemannian
Finsler manifolds
geodesics
Finsler function

adding to it
dynamic covariant derivative
another paper
Kosambi bi-derivative operator
Kosambi

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