L-4: Difference between revisions
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</math></center> | </math></center> | ||
== The second moment == | === The second moment === | ||
==== Exercise: L-4==== | |||
* Step 1: The second moment is | * Step 1: The second moment is | ||
<center> <math> | <center> <math> | ||
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</math></center> | </math></center> | ||
Hence, the quantity <math>\overline{Z[x_t,t]^2}/ (\overline{Z[x_t,t]})^2</math> can be computed. | ====Discussion==== | ||
Hence, the quantity <math>\overline{Z[x_t,t]^2}/ (\overline{Z[x_t,t]})^2</math> can be computed. | |||
* The denominator <math>\int_{u(0)=0}^{u(t)=0} {\cal D} u \exp\left[- \int_0^t d \tau \frac{1}{4T}(\partial_\tau u)^2\right] </math> is the free propagator and gives a contribution <math> \sim =\sqrt{4 T t}. | |||
* Let us define the numerator | |||
<center> <math> | <center> <math> | ||
W(0,t)\int_{u(0)=0}^{u(t)=0} {\cal D} u \exp\left[- \int_0^t d \tau \frac{1}{4T}(\partial_\tau u)^2- \frac{D}{T^2} \delta^d[u(\tau)]\right] | W(0,t)= \int_{u(0)=0}^{u(t)=0} {\cal D} u \exp\left[- \int_0^t d \tau \frac{1}{4T}(\partial_\tau u)^2- \frac{D}{T^2} \delta^d[u(\tau)]\right] | ||
</math></center> | </math></center> | ||
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</math>. | </math>. | ||
The condition above is sufficient but not necessary. It is enough that <math> | The condition above is sufficient but not necessary. It is enough that <math> | ||
\overline{Z[x_t,t]^2}/ (\overline{Z[x_t,t]})^2 <\text{const | \overline{Z[x_t,t]^2}/ (\overline{Z[x_t,t]})^2 <\text{const} </math>, when <math> t\to \infty</math>, to have the equivalence between annealed and quenched averages. | ||
<Strong>Remark II:</Strong> From L-3, we derive using Feynman-Kac, the following equation | <Strong>Remark II:</Strong> From L-3, we derive using Feynman-Kac, the following equation | ||
<center> <math> | <center> <math> | ||
\partial_t W(x,t) =- \hat H W(x,t) | \partial_t W(x,t) =- \hat H W(x,t) | ||
</math></center> | </math></center> | ||
Now the Hamiltonian reads: | Now the Hamiltonian reads: | ||
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H= -2 T \nabla^2 - \frac{D}{T^2} \delta^d[u] | H= -2 T \nabla^2 - \frac{D}{T^2} \delta^d[u] | ||
</math></center> | </math></center> | ||
Now the Hamiltonian is time independent: | |||
<center> <math> | |||
W(x,t) = \langle x|\exp\left( - \hat H t\rangle) |0\rangle | |||
</math></center> | |||
At large times the behaviour is dominatate by the low energy part of the spectrum |
Revision as of 16:43, 11 February 2024
Goal : final lecture on KPZ and directed polymers at finite dimension. We will show that for a "glass transition" takes place.
KPZ : from to the Cayley tree
We know a lot about KPZ, but still we have much to understand:
- In we found and a glassy regime present at all temperatures. The stationary solution of the KPZ equation describes, at long times, the fluctions of quantities like . However it does not identify the actual distribution of for a given . In particular we have no idea from where Tracy Widom comes from.
- In , there is an exact solution for the Cayley tree that predicts a freezing transition to an 1RSB phase ().
- In finite dimension, but larger than 1, there are no exact solutions. Numerical simulations find in . The case Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle d>2} is very interesting.
Let's do replica!
To make progress in disordered systems we have to go through the moments of the partition function. For simplicity we consider polymers starting in Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle 0} and ending in Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle x} . We recall that
- is a Gaussian field with
- From the Wick theorem, for a generic Gaussian Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle W } field we have
The first moment
The first moment of the partition function is
Note that the term Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle T^2 \overline{W^2} = \int d \tau_1 d\tau_2 \overline{V(x,\tau_1)V(x,\tau_2)}= D t \delta_0} has a short distance divergence due to the delta-function. Hence we can write:
The second moment
Exercise: L-4
- Step 1: The second moment is
- Step 2: Use Wick and derive:
- Step 3: Now change coordinate and get:
Discussion
Hence, the quantity Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \overline{Z[x_t,t]^2}/ (\overline{Z[x_t,t]})^2} can be computed.
- The denominator is the free propagator and gives a contribution Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \sim =\sqrt{4 T t}. * Let us define the numerator <center> <math> W(0,t)= \int_{u(0)=0}^{u(t)=0} {\cal D} u \exp\left[- \int_0^t d \tau \frac{1}{4T}(\partial_\tau u)^2- \frac{D}{T^2} \delta^d[u(\tau)]\right] }
Remark 1: From T-I, remember that if
the partition function is self-averaging and . The condition above is sufficient but not necessary. It is enough that Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \overline{Z[x_t,t]^2}/ (\overline{Z[x_t,t]})^2 <\text{const} } , when Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle t\to \infty} , to have the equivalence between annealed and quenched averages.
Remark II: From L-3, we derive using Feynman-Kac, the following equation
Now the Hamiltonian reads:
Now the Hamiltonian is time independent:
At large times the behaviour is dominatate by the low energy part of the spectrum