Dynamic quantum theory of large additional dimensions for non-massive particles.pdf

Dynamic quantum theory of large additional dimensions for non-massive particles.pdf

  1. 1、本文档共5页,可阅读全部内容。
  2. 2、有哪些信誉好的足球投注网站(book118)网站文档一经付费(服务费),不意味着购买了该文档的版权,仅供个人/单位学习、研究之用,不得用于商业用途,未经授权,严禁复制、发行、汇编、翻译或者网络传播等,侵权必究。
  3. 3、本站所有内容均由合作方或网友上传,本站不对文档的完整性、权威性及其观点立场正确性做任何保证或承诺!文档内容仅供研究参考,付费前请自行鉴别。如您付费,意味着您自己接受本站规则且自行承担风险,本站不退款、不进行额外附加服务;查看《如何避免下载的几个坑》。如果您已付费下载过本站文档,您可以点击 这里二次下载
  4. 4、如文档侵犯商业秘密、侵犯著作权、侵犯人身权等,请点击“版权申诉”(推荐),也可以打举报电话:400-050-0827(电话支持时间:9:00-18:30)。
查看更多
Dynamic quantum theory of large additional dimensions for non-massive particles

a r X i v : g r - q c / 0 5 0 1 0 5 6 v 1 1 9 J a n 2 0 0 5 Dynamic quantum theory of large additional dimensions S.N. Andrianov, V.V. Bochkarev Scientific Center for Gravitational Wave Research Dulkyn, Kazan, Russia The Klein-Gordon equation is known in quantum field theory that does not account the changes of space metrics and changes of particles behavior connected with it [1]. Such dynamics is describing by Einsteins equation or Brans-Dicke equation [2]. Wheeler de Witt occupies place of these equations in quantum theory that is generalization of Klein-Gordon equation for the case of general relativity theory and is valid for arbitrary Ryman space [3]. The approach of Wheeler de Witt is applied to brane theory of Universe in paper [4]. However, the variation of bran topology is not accounted in this paper. The variation of space topology is considered in phenomenological way for quantum theory in paper [5]. In paper [6], Wheeler de Witt equation is obtained from priori taken action for inflating brane. In present paper, we will derive equation of Wheeler de Witt type in the framework of brane model with the account of its topology variation in universal space starting from the well-known conservation laws inside brane. It is known that the value pip i conserves at Lorenz transform where pi is four-dimensional momentum of a particle [7]. With that, the following conservation law pip i = 0, (1) is valid for non-massive particle. The three-component vector of momen- tum can be written in non-relativistic quantum mechanics in operator form as ?→p = ?ih??. The evident generalization for four-component case is the value p = ( 1 c H?,?→p ) . (2) 1 where H? is operator of Hamilton since H?ψ = ih??ψ ?t according temporal Schro?dinger equation. Momentum can be expressed in curvilinear coordi- nates as covariant derivative p?i = ?ih? {...};i (3) Lets consider non-mass particle in the three-dimensional Ryman space (brane) immersed in Deckard space-time of higher dimens

文档评论(0)

l215322 + 关注
实名认证
内容提供者

该用户很懒,什么也没介绍

1亿VIP精品文档

相关文档