lecture08 't hooft counting

lecture08 't hooft counting

ID:14362685

大小:232.96 KB

页数:9页

时间:2018-07-28

lecture08 't hooft counting_第1页
lecture08 't hooft counting_第2页
lecture08 't hooft counting_第3页
lecture08 't hooft counting_第4页
lecture08 't hooft counting_第5页
资源描述:

《lecture08 't hooft counting》由会员上传分享,免费在线阅读,更多相关内容在学术论文-天天文库

1、MITOpenCourseWarehttp://ocw.mit.edu8.821StringTheoryFall2008ForinformationaboutcitingthesematerialsorourTermsofUse,visit:http://ocw.mit.edu/terms.8.821F2008Lecture8:LargeNCountingLecturer:McGreevyOctober4,20081IntroductionTodaywe’llcontinueourdiscussionoflargeNscalinginthet

2、’Hooftlimitofquantummatrixmodels.Inparticular,we’llreviewtheNcountingforvacuumdiagramsandlearnhowtodoNcountingforcorrelators.OurperspectiveonthelargeNlimitcontinuestobeoneofconvenience.Itisoneofseveralassumptionsthatenablethesimplestrealizationofholographyandgauge/gravitydu

3、ality.Nexttimewe’llcontinuetalkingaboutsimplifyingassumptionsandturnourattentiontoconformalinvariance.2Vacuumt’HooftcountingLet’srecallourstartingpoint.Wewerethinkingaboutmatrixfieldtheories,fieldtheoriesinwhichallthefieldsareNxNmatricesinadditiontowhateverotherlabelstheymayha

4、ve.Inparticular,wewriteourtheoryschematicallyintermsofonebigfieldΦwhichwethinkofaspotentiallyincludingscalarsφ,gaugefieldsAµ,andfermionsψαallofwhichareNxNmatrices.TheschematicLagrangianis1L=Tr(∂Φ∂Φ−V(Φ))(1)g2whereV(Φ)∼Φ2+Φ4+...andallproductsshouldbethoughtofasmatrixproducts.T

5、hisschematicrepresentationismeanttoconveytwopiecesofinformation.First,thattheLagrangianisinvariantunderU(N)rotationswhichactonthematrixfieldsbyconjugation:Φ→UΦU−1.Second,thatthefieldsarescaledsothatthecouplingg2sitsoutinfrontoftheentireLagrangian.Inparticular,wehavetoverycare

6、fulaboutfieldnormalizationswhendoinglargeNcountingforcorrelationfunctions.Thet’HooftlimitisthelimitwhereN→∞andg2→0whileλ=g2Nremainsfixed.λisthet’Hooftcoupling.NotethatweareadoptingadifferentnormalizationconditionthaninthepreviouslectureonlargeNcounting(thereweusedthefieldΦ˜=(1/

7、g)Φwhichhadkinetictermswiththeusualfieldtheorynormalization).Withourcurrentnormalizationthepropagator�ΦΦ�goeslikeg2=λ.NThepropagatorinthedoublelinenotationappearsinFig.1.Rememberthatforthepurposesof1Figure1:Propagator,λ/NFigure2:Threepointvertex,N/λlargeNcountingweareinstruc

8、tedtothinkonlyaboutcountingpowersofN,sowewillsuppresspositionsoffields,spinindices,

当前文档最多预览五页,下载文档查看全文

此文档下载收益归作者所有

当前文档最多预览五页,下载文档查看全文
温馨提示:
1. 部分包含数学公式或PPT动画的文件,查看预览时可能会显示错乱或异常,文件下载后无此问题,请放心下载。
2. 本文档由用户上传,版权归属用户,天天文库负责整理代发布。如果您对本文档版权有争议请及时联系客服。
3. 下载前请仔细阅读文档内容,确认文档内容符合您的需求后进行下载,若出现内容与标题不符可向本站投诉处理。
4. 下载文档时可能由于网络波动等原因无法下载或下载错误,付费完成后未能成功下载的用户请联系客服处理。