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2 values
$S(\phi )$
$ S ( \phi ) $
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embedded
$\phi $
$ \phi $
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embedded
$\exp (-Ht)$
$ e x p ( - H t ) $
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embedded
$\psi (x)$
$ \psi ( x ) $
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embedded
$d\mu $
$ d \mu $
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embedded
$x$
$ x $
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embedded
$x(t)$
$ x ( t ) $
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embedded
$V$
$ V $
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embedded
$H= L +V(x)$
$ H = L + V ( x ) $
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$L$
$ L $
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$x(t)$
$ x ( t ) $
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\begin {equation} H = \half p^2 + V(x) \end {equation}
\begin{equation*} H = \frac { 1 } { 2 } p ^ { 2 } + V ( x ) \end{equation*}
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isolated
\begin {equation}\label {EVeq} \exp (-Ht) \psi (x) = \int d\mu \exp \left ( -\int _0^t V((x(s)) ds \right ) \psi (x(t)) \end {equation}
\begin{equation*} \operatorname { e x p } ( - H t ) \psi ( x ) = \int d \mu \operatorname { e x p } ( - \int _ { 0 } ^ { t } V ( ( x ( s ) ) d s ) \psi ( x ( t ) ) \end{equation*}
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$x: I \to M$
$ x : I \rightarrow M $
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embedded
$I$
$ I $
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embedded
$[0,t]$
$ [ 0 , t ] $
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embedded
$M$
$ M $
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embedded
$n$
$ n $
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embedded
$g$
$ g $
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embedded
$\omega =dh$
$ \omega = d h $
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embedded
$M$
$ M $
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embedded
$\omega = \Omu (x) d\Xmu $
$ \omega = \omega _ { \mu } ( x ) d x ^ { \mu } $
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$\omega = \Omu (x) d\Xmu $
$ \omega = \omega _ { \mu } ( x ) d x ^ { \mu } $
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$\dot {x}^{\mu }(t')= \frac {d{x}^{\mu }}{d t'}$
$ \dot { x } ^ { \mu } ( t ^ { \prime } ) = \frac { d x ^ { \mu } } { d t ^ { \prime } } $
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$S[x(.)] = i(h(x(t))-h(x(0)))$
$ S [ x ( . ) ] = i ( h ( x ( t ) ) - h ( x ( 0 ) ) ) $
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embedded
$x(t)$
$ x ( t ) $
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embedded
$\omega =0$
$ \omega = 0 $
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embedded
$h$
$ h $
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embedded
$M$
$ M $
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embedded
$\omega =dh$
$ \omega = d h $
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embedded
$\Pmu $
$ p _ { \mu } $
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embedded
$\Xmu $
$ x ^ { \mu } $
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embedded
$n$
$ n $
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embedded
$H(p,x)= \Pmu \Xmu - \Lag (x,\dot {x})$
$ H ( p , x ) = p _ { \mu } x ^ { \mu } - L ( x , \dot { x } ) $
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$H(p,x)= \Pmu \Xmu - \Lag (x,\dot {x})$
$ H ( p , x ) = p _ { \mu } x ^ { \mu } - L ( x , \dot { x } ) $
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$\omega $
$ \omega $
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embedded
$\Pb {\Tmu }{T_{\nu }}=0$
$ \{ T _ { \mu } , T _ { \nu } \} = 0 $
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embedded
$\Pb {\Tmu }{H_c}=0$
$ \{ T _ { \mu } , H _ { c } \} = 0 $
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embedded
$\Tmu $
$ T _ { \mu } $
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embedded
$\psi (x)$
$ \psi ( x ) $
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embedded
$\Pmu =-i \Dmu $
$ p _ { \mu } = - i \partial _ { \mu } $
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embedded
$\Pmu $
$ p _ { \mu } $
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embedded
$-i\DDmu $
$ - i \nabla _ { \mu } $
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embedded
$\XXmu \psi =0$
$ X ^ { \mu } \psi = 0 $
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embedded
$\XXmu =g^{\mu \nu } (p_{\nu } + i\omega _{\nu })$
$ X ^ { \mu } = g ^ { \mu \nu } ( p _ { \nu } + i \omega _ { \nu } ) $
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\begin {equation}\label {ACeq} S[x(.)] = \Intot i\Omu (x(t'))\dot {x}^{\mu }(t') \, dt' \end {equation}
\begin{equation*} S [ x ( . ) ] = \int _ { 0 } ^ { t } i \omega _ { \mu } ( x ( t ^ { \prime } ) ) \dot { x } ^ { \mu } ( t ^ { \prime } ) \, d t ^ { \prime } \end{equation*}
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isolated
\begin {equation}\label {MOMeq} \Pmu = \frac {\delta \Lag }{\delta \dot {x}^\mu } = i\Omu , \end {equation}
\begin{equation*} p _ { \mu } = \frac { \delta L } { \delta \dot { x } ^ { \mu } } = i \omega _ { \mu } , \end{equation*}
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isolated
\begin {equation} \Tmu \equiv \Pmu - i\Omu . \end {equation}
\begin{equation*} T _ { \mu } \equiv p _ { \mu } - i \omega _ { \mu } . \end{equation*}
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isolated
\begin {equation}\label {GTeq} \delta _{\epsilon }\psi (x) =-i \epsilon (\Dmu \psi (x) + \Omu (x) \psi (x)) \end {equation}
\begin{equation*} \delta _ { \epsilon } \psi ( x ) = - i \epsilon ( \partial _ { \mu } \psi ( x ) + \omega _ { \mu } ( x ) \psi ( x ) ) \end{equation*}
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isolated
$\Etamu $
$ \eta ^ { \mu } $
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embedded
$\Pimu $
$ \pi _ { \mu } $
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embedded
$(2n,2n)$
$ ( 2 n , 2 n ) $
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embedded
$\Etamu ,\Pimu $
$ \eta ^ { \mu } , \pi _ { \mu } $
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embedded
$\nabla $
$ \nabla $
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embedded
$\psi (x,\eta )$
$ \psi ( x , \eta ) $
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embedded
$\Pmu =-i \DDmu $
$ p _ { \mu } = - i \nabla _ { \mu } $
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embedded
$\Pimu = -i\frac {\partial }{\partial \Etamu }$
$ \pi _ { \mu } = - i \frac { \partial } { \partial \eta ^ { \mu } } $
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embedded
$\psi (x,\eta )$
$ \psi ( x , \eta ) $
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embedded
$(n,n)$
$ ( n , n ) $
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embedded
$SM$
$ S M $
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embedded
$\Xmu ,\Etamu $
$ x ^ { \mu } , \eta ^ { \mu } $
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embedded
$Q$
$ Q $
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embedded
$Q=\Etamu \Tmu =-i\Etamu (\Dmu + \omega )$
$ Q = \eta ^ { \mu } T _ { \mu } = - i \eta ^ { \mu } ( \partial _ { \mu } + \omega ) $
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$Q=\Etamu \Tmu =-i\Etamu (\Dmu + \omega )$
$ Q = \eta ^ { \mu } T _ { \mu } = - i \eta ^ { \mu } ( \partial _ { \mu } + \omega ) $
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$\chi $
$ \chi $
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embedded
$\chi = \Pimu \XXmu = -ig^{\mu \nu } \Pimu (\nabla _{\nu }-\omega _{\nu })$
$ \chi = \pi _ { \mu } X ^ { \mu } = - i g ^ { \mu \nu } \pi _ { \mu } ( \nabla _ { \nu } - \omega _ { \nu } ) $
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$M$
$ M $
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embedded
$\psi (x,\eta )$
$ \psi ( x , \eta ) $
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embedded
$Q=-i\Emh d \Eph $
$ Q = - i e ^ { - h } d e ^ { h } $
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embedded
$\chi = \Eph \delta \Emh $
$ \chi = e ^ { h } \delta e ^ { - h } $
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embedded
$d$
$ d $
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embedded
$\delta = *d*$
$ \delta = \ast d \ast $
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embedded
$h$
$ h $
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embedded
$\chi =\Pimu \XXmu $
$ \chi = \pi _ { \mu } X ^ { \mu } $
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embedded
$h$
$ h $
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embedded
$Q$
$ Q $
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embedded
$h$
$ h $
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embedded
$H_g$
$ H _ { g } $
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embedded
\begin {equation}\label {SPBeq} d\Pmu \wedge d \Xmu + \nabla \Pimu \wedge \nabla \Etamu + \frac 12 dx^{\mu } \wedge dx^{\nu } \Curv {\mu }{\nu }{\kappa }{\lambda }\eta ^{\kappa }\pi _{\lambda }, \end {equation}
\begin{equation*} d p _ { \mu } \wedge d x ^ { \mu } + \nabla \pi _ { \mu } \wedge \nabla \eta ^ { \mu } + \frac { 1 } { 2 } d x ^ { \mu } \wedge d x ^ { \nu } R _ { \mu \nu \kappa } { } ^ { \lambda } \eta ^ { \kappa } \pi _ { \lambda } , \end{equation*}
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isolated
\begin {eqnarray}\DDmu \psi (x,\eta ) = \Dmu \psi (x,\eta ) + \Gam {\mu }{\nu }{\lambda } \eta ^{\nu } \frac {\partial }{\partial \eta ^{\lambda }}\psi (x,\eta ). \end {eqnarray}
\begin{equation*} \nabla _ { \mu } \psi ( x , \eta ) = \partial _ { \mu } \psi ( x , \eta ) + \Gamma _ { \mu \nu } ^ { \lambda } \eta ^ { \nu } \frac { \partial } { \partial \eta ^ { \lambda } } \psi ( x , \eta ) . \end{equation*}
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isolated
\begin {eqnarray}H_g &=& i( Q \chi + \chi Q) \End &=& d \delta + \delta d + g^{\mu \nu }\Omu \omega _{\nu } -i (\Pimu \eta ^{\nu } - \eta ^{\nu }\Pimu ) \frac {\partial ^2 h }{\partial \Xmu \partial x_{\nu }}. \end {eqnarray}
\begin{align*} H _ { g } & = & i ( Q \chi + \chi Q ) \\ & = & d \delta + \delta d + g ^ { \mu \nu } \omega _ { \mu } \omega _ { \nu } - i ( \pi _ { \mu } \eta ^ { \nu } - \eta ^ { \nu } \pi _ { \mu } ) \frac { \partial ^ { 2 } h } { \partial x ^ { \mu } \partial x _ { \nu } } . \end{align*}
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isolated
$H_g$
$ H _ { g } $
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embedded
$x_t,\eta _t$
$ x _ { t } , \eta _ { t } $
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embedded
$SM$
$ S M $
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embedded
$\Xmu ,\Etamu $
$ x ^ { \mu } , \eta ^ { \mu } $
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embedded
$b_t$
$ b _ { t } $
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embedded
$(\theta _t,\rho _t)$
$ ( \theta _ { t } , \rho _ { t } ) $
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embedded
$(d+ \delta )^2$
$ ( d + \delta ) ^ { 2 } $
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embedded
$J$
$ J $
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embedded
$u:\Sigma \to M$
$ u : \Sigma \rightarrow M $
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embedded
$\Sigma $
$ \Sigma $
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embedded
$2m$
$ 2 m $
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embedded
$M$
$ M $
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embedded
$H^{\alpha }_{\mu }$
$ H _ { \mu } ^ { \alpha } $
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embedded
$\Etamu $
$ \eta ^ { \mu } $
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embedded
$\pi ^{\alpha }_{\mu }$
$ \pi _ { \mu } ^ { \alpha } $
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embedded
$\alpha =1,2$
$ \alpha = 1 , 2 $
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embedded
$\Sigma $
$ \Sigma $
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embedded
$\mu =1,\dots ,2 m$
$ \mu = 1 , \ldots , 2 m $
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embedded
$M$
$ M $
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embedded