mirror of
https://github.com/TREX-CoE/qmc-lttc.git
synced 2024-09-16 17:55:31 +02:00
PDMC OK
This commit is contained in:
parent
f9354e4401
commit
ca11c6c032
201
QMC.org
201
QMC.org
@ -1,9 +1,7 @@
|
||||
#+TITLE: Quantum Monte Carlo
|
||||
#+AUTHOR: Anthony Scemama, Claudia Filippi
|
||||
# SETUPFILE: https://fniessen.github.io/org-html-themes/org/theme-readtheorg.setup
|
||||
# SETUPFILE: https://fniessen.github.io/org-html-themes/org/theme-bigblow.setup
|
||||
#+LANGUAGE: en
|
||||
#+INFOJS_OPT: toc:t mouse:underline path:http://orgmode.org/org-info.js
|
||||
#+INFOJS_OPT: toc:t mouse:underline path:org-info.js
|
||||
#+STARTUP: latexpreview
|
||||
#+LATEX_CLASS: report
|
||||
#+LATEX_HEADER_EXTRA: \usepackage{minted}
|
||||
@ -47,7 +45,7 @@
|
||||
computes a statistical estimate of the expectation value of the energy
|
||||
associated with a given wave function.
|
||||
Finally, we introduce the diffusion Monte Carlo (DMC) method which
|
||||
gives the exact energy of the hydrogen atom and of the $H_2$ molecule.
|
||||
gives the exact energy of the hydrogen atom and of the H_2 molecule.
|
||||
|
||||
Code examples will be given in Python and Fortran. You can use
|
||||
whatever language you prefer to write the program.
|
||||
@ -1156,17 +1154,17 @@ gfortran hydrogen.f90 qmc_stats.f90 qmc_uniform.f90 -o qmc_uniform
|
||||
initial position $\mathbf{r}_0$, we will realize a random walk as follows:
|
||||
|
||||
$$
|
||||
\mathbf{r}_{n+1} = \mathbf{r}_{n} + \tau \mathbf{u}
|
||||
\mathbf{r}_{n+1} = \mathbf{r}_{n} + \delta t\, \mathbf{u}
|
||||
$$
|
||||
|
||||
where $\tau$ is a fixed constant (the so-called /time-step/), and
|
||||
where $\delta t$ is a fixed constant (the so-called /time-step/), and
|
||||
$\mathbf{u}$ is a uniform random number in a 3-dimensional box
|
||||
$(-1,-1,-1) \le \mathbf{u} \le (1,1,1)$. We will then add the
|
||||
accept/reject step that guarantees that the distribution of the
|
||||
$\mathbf{r}_n$ is $\Psi^2$:
|
||||
|
||||
1) Compute $\Psi$ at a new position $\mathbf{r'} = \mathbf{r}_n +
|
||||
\tau \mathbf{u}$
|
||||
\delta t\, \mathbf{u}$
|
||||
2) Compute the ratio $R = \frac{\left[\Psi(\mathbf{r'})\right]^2}{\left[\Psi(\mathbf{r}_{n})\right]^2}$
|
||||
3) Draw a uniform random number $v \in [0,1]$
|
||||
4) if $v \le R$, accept the move : set $\mathbf{r}_{n+1} = \mathbf{r'}$
|
||||
@ -1213,15 +1211,15 @@ gfortran hydrogen.f90 qmc_stats.f90 qmc_uniform.f90 -o qmc_uniform
|
||||
from hydrogen import *
|
||||
from qmc_stats import *
|
||||
|
||||
def MonteCarlo(a,nmax,tau):
|
||||
def MonteCarlo(a,nmax,dt):
|
||||
# TODO
|
||||
return energy/nmax, N_accep/nmax
|
||||
|
||||
# Run simulation
|
||||
a = 0.9
|
||||
nmax = 100000
|
||||
tau = 1.3
|
||||
X0 = [ MonteCarlo(a,nmax,tau) for i in range(30)]
|
||||
dt = 1.3
|
||||
X0 = [ MonteCarlo(a,nmax,dt) for i in range(30)]
|
||||
|
||||
# Energy
|
||||
X = [ x for (x, _) in X0 ]
|
||||
@ -1236,11 +1234,11 @@ print(f"A = {A} +/- {deltaA}")
|
||||
|
||||
*Fortran*
|
||||
#+BEGIN_SRC f90 :tangle none
|
||||
subroutine metropolis_montecarlo(a,nmax,tau,energy,accep)
|
||||
subroutine metropolis_montecarlo(a,nmax,dt,energy,accep)
|
||||
implicit none
|
||||
double precision, intent(in) :: a
|
||||
integer*8 , intent(in) :: nmax
|
||||
double precision, intent(in) :: tau
|
||||
double precision, intent(in) :: dt
|
||||
double precision, intent(out) :: energy
|
||||
double precision, intent(out) :: accep
|
||||
|
||||
@ -1257,7 +1255,7 @@ end subroutine metropolis_montecarlo
|
||||
program qmc
|
||||
implicit none
|
||||
double precision, parameter :: a = 0.9d0
|
||||
double precision, parameter :: tau = 1.3d0
|
||||
double precision, parameter :: dt = 1.3d0
|
||||
integer*8 , parameter :: nmax = 100000
|
||||
integer , parameter :: nruns = 30
|
||||
|
||||
@ -1266,7 +1264,7 @@ program qmc
|
||||
double precision :: ave, err
|
||||
|
||||
do irun=1,nruns
|
||||
call metropolis_montecarlo(a,nmax,tau,X(irun),Y(irun))
|
||||
call metropolis_montecarlo(a,nmax,dt,X(irun),Y(irun))
|
||||
enddo
|
||||
|
||||
call ave_error(X,nruns,ave,err)
|
||||
@ -1288,13 +1286,13 @@ gfortran hydrogen.f90 qmc_stats.f90 qmc_metropolis.f90 -o qmc_metropolis
|
||||
from hydrogen import *
|
||||
from qmc_stats import *
|
||||
|
||||
def MonteCarlo(a,nmax,tau):
|
||||
def MonteCarlo(a,nmax,dt):
|
||||
energy = 0.
|
||||
N_accep = 0
|
||||
r_old = np.random.uniform(-tau, tau, (3))
|
||||
r_old = np.random.uniform(-dt, dt, (3))
|
||||
psi_old = psi(a,r_old)
|
||||
for istep in range(nmax):
|
||||
r_new = r_old + np.random.uniform(-tau,tau,(3))
|
||||
r_new = r_old + np.random.uniform(-dt,dt,(3))
|
||||
psi_new = psi(a,r_new)
|
||||
ratio = (psi_new / psi_old)**2
|
||||
v = np.random.uniform()
|
||||
@ -1308,8 +1306,8 @@ def MonteCarlo(a,nmax,tau):
|
||||
# Run simulation
|
||||
a = 0.9
|
||||
nmax = 100000
|
||||
tau = 1.3
|
||||
X0 = [ MonteCarlo(a,nmax,tau) for i in range(30)]
|
||||
dt = 1.3
|
||||
X0 = [ MonteCarlo(a,nmax,dt) for i in range(30)]
|
||||
|
||||
# Energy
|
||||
X = [ x for (x, _) in X0 ]
|
||||
@ -1328,11 +1326,11 @@ print(f"A = {A} +/- {deltaA}")
|
||||
|
||||
*Fortran*
|
||||
#+BEGIN_SRC f90 :exports code
|
||||
subroutine metropolis_montecarlo(a,nmax,tau,energy,accep)
|
||||
subroutine metropolis_montecarlo(a,nmax,dt,energy,accep)
|
||||
implicit none
|
||||
double precision, intent(in) :: a
|
||||
integer*8 , intent(in) :: nmax
|
||||
double precision, intent(in) :: tau
|
||||
double precision, intent(in) :: dt
|
||||
double precision, intent(out) :: energy
|
||||
double precision, intent(out) :: accep
|
||||
|
||||
@ -1346,11 +1344,11 @@ subroutine metropolis_montecarlo(a,nmax,tau,energy,accep)
|
||||
energy = 0.d0
|
||||
n_accep = 0_8
|
||||
call random_number(r_old)
|
||||
r_old(:) = tau * (2.d0*r_old(:) - 1.d0)
|
||||
r_old(:) = dt * (2.d0*r_old(:) - 1.d0)
|
||||
psi_old = psi(a,r_old)
|
||||
do istep = 1,nmax
|
||||
call random_number(r_new)
|
||||
r_new(:) = r_old(:) + tau * (2.d0*r_new(:) - 1.d0)
|
||||
r_new(:) = r_old(:) + dt * (2.d0*r_new(:) - 1.d0)
|
||||
psi_new = psi(a,r_new)
|
||||
ratio = (psi_new / psi_old)**2
|
||||
call random_number(v)
|
||||
@ -1368,7 +1366,7 @@ end subroutine metropolis_montecarlo
|
||||
program qmc
|
||||
implicit none
|
||||
double precision, parameter :: a = 0.9d0
|
||||
double precision, parameter :: tau = 1.3d0
|
||||
double precision, parameter :: dt = 1.3d0
|
||||
integer*8 , parameter :: nmax = 100000
|
||||
integer , parameter :: nruns = 30
|
||||
|
||||
@ -1377,7 +1375,7 @@ program qmc
|
||||
double precision :: ave, err
|
||||
|
||||
do irun=1,nruns
|
||||
call metropolis_montecarlo(a,nmax,tau,X(irun),Y(irun))
|
||||
call metropolis_montecarlo(a,nmax,dt,X(irun),Y(irun))
|
||||
enddo
|
||||
|
||||
call ave_error(X,nruns,ave,err)
|
||||
@ -1477,12 +1475,12 @@ end subroutine random_gauss
|
||||
|
||||
Now, if instead of drawing uniform random numbers we
|
||||
choose to draw Gaussian random numbers with zero mean and variance
|
||||
$\tau$, the transition probability becomes:
|
||||
$\delta t$, the transition probability becomes:
|
||||
|
||||
\[
|
||||
T(\mathbf{r}_{n} \rightarrow \mathbf{r}_{n+1}) =
|
||||
\frac{1}{(2\pi\,\tau)^{3/2}} \exp \left[ - \frac{\left(
|
||||
\mathbf{r}_{n+1} - \mathbf{r}_{n} \right)^2}{2\tau} \right]
|
||||
\frac{1}{(2\pi\,\delta t)^{3/2}} \exp \left[ - \frac{\left(
|
||||
\mathbf{r}_{n+1} - \mathbf{r}_{n} \right)^2}{2\delta t} \right]
|
||||
\]
|
||||
|
||||
|
||||
@ -1500,19 +1498,19 @@ end subroutine random_gauss
|
||||
The numerical scheme becomes a drifted diffusion:
|
||||
|
||||
\[
|
||||
\mathbf{r}_{n+1} = \mathbf{r}_{n} + \tau \frac{\nabla
|
||||
\mathbf{r}_{n+1} = \mathbf{r}_{n} + \delta t\, \frac{\nabla
|
||||
\Psi(\mathbf{r})}{\Psi(\mathbf{r})} + \chi
|
||||
\]
|
||||
|
||||
where $\chi$ is a Gaussian random variable with zero mean and
|
||||
variance $\tau$.
|
||||
variance $\delta t$.
|
||||
The transition probability becomes:
|
||||
|
||||
\[
|
||||
T(\mathbf{r}_{n} \rightarrow \mathbf{r}_{n+1}) =
|
||||
\frac{1}{(2\pi\,\tau)^{3/2}} \exp \left[ - \frac{\left(
|
||||
\frac{1}{(2\pi\,\delta t)^{3/2}} \exp \left[ - \frac{\left(
|
||||
\mathbf{r}_{n+1} - \mathbf{r}_{n} - \frac{\nabla
|
||||
\Psi(\mathbf{r}_n)}{\Psi(\mathbf{r}_n)} \right)^2}{2\,\tau} \right]
|
||||
\Psi(\mathbf{r}_n)}{\Psi(\mathbf{r}_n)} \right)^2}{2\,\delta t} \right]
|
||||
\]
|
||||
|
||||
|
||||
@ -1570,14 +1568,14 @@ end subroutine drift
|
||||
from hydrogen import *
|
||||
from qmc_stats import *
|
||||
|
||||
def MonteCarlo(a,nmax,tau):
|
||||
def MonteCarlo(a,nmax,dt):
|
||||
# TODO
|
||||
|
||||
# Run simulation
|
||||
a = 0.9
|
||||
nmax = 100000
|
||||
tau = 1.3
|
||||
X0 = [ MonteCarlo(a,nmax,tau) for i in range(30)]
|
||||
dt = 1.3
|
||||
X0 = [ MonteCarlo(a,nmax,dt) for i in range(30)]
|
||||
|
||||
# Energy
|
||||
X = [ x for (x, _) in X0 ]
|
||||
@ -1592,14 +1590,14 @@ print(f"A = {A} +/- {deltaA}")
|
||||
|
||||
*Fortran*
|
||||
#+BEGIN_SRC f90 :tangle none
|
||||
subroutine variational_montecarlo(a,tau,nmax,energy,accep_rate)
|
||||
subroutine variational_montecarlo(a,dt,nmax,energy,accep_rate)
|
||||
implicit none
|
||||
double precision, intent(in) :: a, tau
|
||||
double precision, intent(in) :: a, dt
|
||||
integer*8 , intent(in) :: nmax
|
||||
double precision, intent(out) :: energy, accep_rate
|
||||
|
||||
integer*8 :: istep
|
||||
double precision :: sq_tau, chi(3)
|
||||
double precision :: sq_dt, chi(3)
|
||||
double precision :: psi_old, psi_new
|
||||
double precision :: r_old(3), r_new(3)
|
||||
double precision :: d_old(3), d_new(3)
|
||||
@ -1612,7 +1610,7 @@ end subroutine variational_montecarlo
|
||||
program qmc
|
||||
implicit none
|
||||
double precision, parameter :: a = 0.9
|
||||
double precision, parameter :: tau = 1.0
|
||||
double precision, parameter :: dt = 1.0
|
||||
integer*8 , parameter :: nmax = 100000
|
||||
integer , parameter :: nruns = 30
|
||||
|
||||
@ -1621,7 +1619,7 @@ program qmc
|
||||
double precision :: ave, err
|
||||
|
||||
do irun=1,nruns
|
||||
call variational_montecarlo(a,tau,nmax,X(irun),accep(irun))
|
||||
call variational_montecarlo(a,dt,nmax,X(irun),accep(irun))
|
||||
enddo
|
||||
call ave_error(X,nruns,ave,err)
|
||||
print *, 'E = ', ave, '+/-', err
|
||||
@ -1641,23 +1639,23 @@ gfortran hydrogen.f90 qmc_stats.f90 vmc_metropolis.f90 -o vmc_metropolis
|
||||
from hydrogen import *
|
||||
from qmc_stats import *
|
||||
|
||||
def MonteCarlo(a,nmax,tau):
|
||||
def MonteCarlo(a,nmax,dt):
|
||||
energy = 0.
|
||||
accep_rate = 0.
|
||||
sq_tau = np.sqrt(tau)
|
||||
sq_dt = np.sqrt(dt)
|
||||
r_old = np.random.normal(loc=0., scale=1.0, size=(3))
|
||||
d_old = drift(a,r_old)
|
||||
d2_old = np.dot(d_old,d_old)
|
||||
psi_old = psi(a,r_old)
|
||||
for istep in range(nmax):
|
||||
chi = np.random.normal(loc=0., scale=1.0, size=(3))
|
||||
r_new = r_old + tau * d_old + sq_tau * chi
|
||||
r_new = r_old + dt * d_old + sq_dt * chi
|
||||
d_new = drift(a,r_new)
|
||||
d2_new = np.dot(d_new,d_new)
|
||||
psi_new = psi(a,r_new)
|
||||
# Metropolis
|
||||
prod = np.dot((d_new + d_old), (r_new - r_old))
|
||||
argexpo = 0.5 * (d2_new - d2_old)*tau + prod
|
||||
argexpo = 0.5 * (d2_new - d2_old)*dt + prod
|
||||
q = psi_new / psi_old
|
||||
q = np.exp(-argexpo) * q*q
|
||||
if np.random.uniform() < q:
|
||||
@ -1673,8 +1671,8 @@ def MonteCarlo(a,nmax,tau):
|
||||
# Run simulation
|
||||
a = 0.9
|
||||
nmax = 100000
|
||||
tau = 1.3
|
||||
X0 = [ MonteCarlo(a,nmax,tau) for i in range(30)]
|
||||
dt = 1.3
|
||||
X0 = [ MonteCarlo(a,nmax,dt) for i in range(30)]
|
||||
|
||||
# Energy
|
||||
X = [ x for (x, _) in X0 ]
|
||||
@ -1693,20 +1691,20 @@ print(f"A = {A} +/- {deltaA}")
|
||||
|
||||
*Fortran*
|
||||
#+BEGIN_SRC f90
|
||||
subroutine variational_montecarlo(a,tau,nmax,energy,accep_rate)
|
||||
subroutine variational_montecarlo(a,dt,nmax,energy,accep_rate)
|
||||
implicit none
|
||||
double precision, intent(in) :: a, tau
|
||||
double precision, intent(in) :: a, dt
|
||||
integer*8 , intent(in) :: nmax
|
||||
double precision, intent(out) :: energy, accep_rate
|
||||
|
||||
integer*8 :: istep
|
||||
double precision :: sq_tau, chi(3), d2_old, prod, u
|
||||
double precision :: sq_dt, chi(3), d2_old, prod, u
|
||||
double precision :: psi_old, psi_new, d2_new, argexpo, q
|
||||
double precision :: r_old(3), r_new(3)
|
||||
double precision :: d_old(3), d_new(3)
|
||||
double precision, external :: e_loc, psi
|
||||
|
||||
sq_tau = dsqrt(tau)
|
||||
sq_dt = dsqrt(dt)
|
||||
|
||||
! Initialization
|
||||
energy = 0.d0
|
||||
@ -1718,7 +1716,7 @@ subroutine variational_montecarlo(a,tau,nmax,energy,accep_rate)
|
||||
|
||||
do istep = 1,nmax
|
||||
call random_gauss(chi,3)
|
||||
r_new(:) = r_old(:) + tau * d_old(:) + chi(:)*sq_tau
|
||||
r_new(:) = r_old(:) + dt * d_old(:) + chi(:)*sq_dt
|
||||
call drift(a,r_new,d_new)
|
||||
d2_new = d_new(1)*d_new(1) + d_new(2)*d_new(2) + d_new(3)*d_new(3)
|
||||
psi_new = psi(a,r_new)
|
||||
@ -1726,7 +1724,7 @@ subroutine variational_montecarlo(a,tau,nmax,energy,accep_rate)
|
||||
prod = (d_new(1) + d_old(1))*(r_new(1) - r_old(1)) + &
|
||||
(d_new(2) + d_old(2))*(r_new(2) - r_old(2)) + &
|
||||
(d_new(3) + d_old(3))*(r_new(3) - r_old(3))
|
||||
argexpo = 0.5d0 * (d2_new - d2_old)*tau + prod
|
||||
argexpo = 0.5d0 * (d2_new - d2_old)*dt + prod
|
||||
q = psi_new / psi_old
|
||||
q = dexp(-argexpo) * q*q
|
||||
call random_number(u)
|
||||
@ -1746,7 +1744,7 @@ end subroutine variational_montecarlo
|
||||
program qmc
|
||||
implicit none
|
||||
double precision, parameter :: a = 0.9
|
||||
double precision, parameter :: tau = 1.0
|
||||
double precision, parameter :: dt = 1.0
|
||||
integer*8 , parameter :: nmax = 100000
|
||||
integer , parameter :: nruns = 30
|
||||
|
||||
@ -1755,7 +1753,7 @@ program qmc
|
||||
double precision :: ave, err
|
||||
|
||||
do irun=1,nruns
|
||||
call variational_montecarlo(a,tau,nmax,X(irun),accep(irun))
|
||||
call variational_montecarlo(a,dt,nmax,X(irun),accep(irun))
|
||||
enddo
|
||||
call ave_error(X,nruns,ave,err)
|
||||
print *, 'E = ', ave, '+/-', err
|
||||
@ -1845,7 +1843,7 @@ gfortran hydrogen.f90 qmc_stats.f90 vmc_metropolis.f90 -o vmc_metropolis
|
||||
- a rate equation for the potential.
|
||||
|
||||
The diffusion equation can be simulated by a Brownian motion:
|
||||
\[ \mathbf{r}_{n+1} = \mathbf{r}_{n} + \sqrt{\tau}\, \chi \]
|
||||
\[ \mathbf{r}_{n+1} = \mathbf{r}_{n} + \sqrt{\delta t}\, \chi \]
|
||||
where $\chi$ is a Gaussian random variable, and the rate equation
|
||||
can be simulated by creating or destroying particles over time (a
|
||||
so-called branching process).
|
||||
@ -1871,7 +1869,7 @@ gfortran hydrogen.f90 qmc_stats.f90 vmc_metropolis.f90 -o vmc_metropolis
|
||||
\left[ -\frac{1}{2} \Delta \psi(\mathbf{r},\tau) + V(\mathbf{r}) \psi(\mathbf{r},\tau) \right] \Psi_T(\mathbf{r})
|
||||
\]
|
||||
|
||||
Defining $\Pi(\mathbf{r},t) = \psi(\mathbf{r},\tau)
|
||||
Defining $\Pi(\mathbf{r},\tau) = \psi(\mathbf{r},\tau)
|
||||
\Psi_T(\mathbf{r})$,
|
||||
|
||||
\[
|
||||
@ -1881,10 +1879,15 @@ gfortran hydrogen.f90 qmc_stats.f90 vmc_metropolis.f90 -o vmc_metropolis
|
||||
\right] + E_L(\mathbf{r}) \Pi(\mathbf{r},\tau)
|
||||
\]
|
||||
|
||||
The new "kinetic energy" can be simulated by the drifted diffusion
|
||||
scheme presented in the previous section (VMC).
|
||||
The new "potential" is the local energy, which has smaller fluctuations
|
||||
as $\Psi_T$ tends to the exact wave function. The new "kinetic energy"
|
||||
can be simulated by the drifted diffusion scheme presented in the
|
||||
previous section (VMC).
|
||||
when $\Psi_T$ gets closer to the exact wave function. It can be simulated by
|
||||
changing the number of particles according to $\exp\left[ -\delta t\,
|
||||
\left(E_L(\mathbf{r}) - E_\text{ref}\right)\right]$
|
||||
where $E_{\text{ref}}$ is a constant introduced so that the average
|
||||
of this term is close to one, keeping the number of particles rather
|
||||
constant.
|
||||
|
||||
This equation generates the /N/-electron density $\Pi$, which is the
|
||||
product of the ground state with the trial wave function. It
|
||||
@ -1895,7 +1898,7 @@ gfortran hydrogen.f90 qmc_stats.f90 vmc_metropolis.f90 -o vmc_metropolis
|
||||
systems where the wave function has nodes (systems with 3 or more
|
||||
electrons), this scheme introduces an error known as the /fixed node
|
||||
error/.
|
||||
|
||||
|
||||
*** Appendix : Details of the Derivation
|
||||
|
||||
\[
|
||||
@ -1942,15 +1945,87 @@ gfortran hydrogen.f90 qmc_stats.f90 vmc_metropolis.f90 -o vmc_metropolis
|
||||
\right] + E_L(\mathbf{r}) \Pi(\mathbf{r},\tau)
|
||||
\]
|
||||
|
||||
|
||||
** Fixed-node DMC energy
|
||||
|
||||
Now that we have a process to sample $\Pi(\mathbf{r},\tau) =
|
||||
\psi(\mathbf{r},\tau) \Psi_T(\mathbf{r})$, we can compute the exact
|
||||
energy of the system, within the fixed-node constraint, as:
|
||||
|
||||
\[
|
||||
E = \lim_{\tau \to \infty} \frac{\int \Pi(\mathbf{r},\tau) E_L(\mathbf{r}) d\mathbf{r}}
|
||||
{\int \Pi(\mathbf{r},\tau) d\mathbf{r}} = \lim_{\tau \to
|
||||
\infty} E(\tau).
|
||||
\]
|
||||
|
||||
Indeed, this is equivalent to
|
||||
|
||||
\[
|
||||
E(\tau) = \frac{\int \psi(\mathbf{r},\tau) \Psi_T(\mathbf{r}) E_L(\mathbf{r}) d\mathbf{r}}
|
||||
{\int \psi(\mathbf{r},\tau) \Psi_T(\mathbf{r}) d\mathbf{r}}
|
||||
= \frac{\int \psi(\mathbf{r},\tau) \hat{H} \Psi_T(\mathbf{r}) d\mathbf{r}}
|
||||
{\int \psi(\mathbf{r},\tau) \Psi_T(\mathbf{r}) d\mathbf{r}}
|
||||
= \frac{\langle \psi_\tau | \hat{H} | \Psi_T \rangle}
|
||||
{\langle \psi_\tau | \Psi_T \rangle}
|
||||
\]
|
||||
|
||||
As $\hat{H}$ is Hermitian,
|
||||
|
||||
\[
|
||||
E(\tau) = \frac{\langle \psi_\tau | \hat{H} | \Psi_T \rangle}
|
||||
{\langle \psi_\tau | \Psi_T \rangle}
|
||||
= \frac{\langle \Psi_T | \hat{H} | \psi_\tau \rangle}
|
||||
{\langle \Psi_T | \psi_\tau \rangle}
|
||||
= E[\psi_\tau] \frac{\langle \Psi_T | \psi_\tau \rangle}
|
||||
{\langle \Psi_T | \psi_\tau \rangle}
|
||||
= E[\psi_\tau]
|
||||
\]
|
||||
|
||||
So computing the energy within DMC consists in generating the
|
||||
density $\Pi$, and simply averaging the local energies computed
|
||||
with the trial wave function.
|
||||
|
||||
** Pure Diffusion Monte Carlo
|
||||
|
||||
Instead of having a variable number of particles to simulate the
|
||||
branching process, one can choose to sample $[\Psi_T(\mathbf{r})]^2$ instead of
|
||||
$\psi(\mathbf{r},\tau) \Psi_T(\mathbf{r})$, and consider the term
|
||||
$\exp \left( -\delta t\,( E_L(\mathbf{r}) - E_{\text{ref}} \right)$ as a
|
||||
cumulative product of branching weights:
|
||||
|
||||
\[
|
||||
W(\mathbf{r}_n, \tau)
|
||||
= \exp \left( \int_0^\tau - (E_L(\mathbf{r}_t) - E_{\text{ref}}) dt \right)
|
||||
\approx \prod_{i=1}^{n} \exp \left( -\delta t\, (E_L(\mathbf{r}_i) - E_{\text{ref}}) \right).
|
||||
\]
|
||||
|
||||
The wave function becomes
|
||||
|
||||
\[
|
||||
\psi(\mathbf{r},\tau) = \Psi_T(\mathbf{r}) W(\mathbf{r},\tau)
|
||||
\]
|
||||
|
||||
and the expression of the fixed-node DMC energy is
|
||||
|
||||
\begin{eqnarray*}
|
||||
E(\tau) & = & \frac{\int \psi(\mathbf{r},\tau) \Psi_T(\mathbf{r}) E_L(\mathbf{r}) d\mathbf{r}}
|
||||
{\int \psi(\mathbf{r},\tau) \Psi_T(\mathbf{r}) d\mathbf{r}} \\
|
||||
& = & \frac{\int \left[ \Psi_T(\mathbf{r}) \right]^2 W(\mathbf{r},\tau) E_L(\mathbf{r}) d\mathbf{r}}
|
||||
{\int \left[ \Psi_T(\mathbf{r}) \right]^2 W(\mathbf{r},\tau) d\mathbf{r}} \\
|
||||
\end{eqnarray*}
|
||||
|
||||
This algorithm is less stable than the branching algorithm: it
|
||||
requires to have a value of $E_\text{ref}$ which is close to the
|
||||
fixed-node energy, and a good trial wave function. Its big
|
||||
advantage is that it is very easy to program starting from a VMC code.
|
||||
|
||||
** TODO Hydrogen atom
|
||||
|
||||
*** Exercise
|
||||
|
||||
#+begin_exercise
|
||||
Modify the Metropolis VMC program to introduce the PDMC weight.
|
||||
In the limit $\tau \rightarrow 0$, you should recover the exact
|
||||
In the limit $\delta t \rightarrow 0$, you should recover the exact
|
||||
energy of H for any value of $a$.
|
||||
#+end_exercise
|
||||
|
||||
@ -2094,7 +2169,7 @@ gfortran hydrogen.f90 qmc_stats.f90 vmc_metropolis.f90 -o vmc_metropolis
|
||||
: A = 0.78861366666666655 +/- 3.5096729498002445E-004
|
||||
|
||||
|
||||
** TODO Dihydrogen
|
||||
** TODO H_2
|
||||
|
||||
We will now consider the H_2 molecule in a minimal basis composed of the
|
||||
$1s$ orbitals of the hydrogen atoms:
|
||||
@ -2108,7 +2183,7 @@ gfortran hydrogen.f90 qmc_stats.f90 vmc_metropolis.f90 -o vmc_metropolis
|
||||
the nuclei.
|
||||
|
||||
|
||||
* Appendix :noexport:
|
||||
* Old sections to be removed :noexport:
|
||||
|
||||
** Gaussian sampling :noexport:
|
||||
:PROPERTIES:
|
||||
|
||||
288
docs/org-info.js
Normal file
288
docs/org-info.js
Normal file
@ -0,0 +1,288 @@
|
||||
function OrgNode(e,h,f,g,d,b,j){var i=this;i.D=e;i.I=b;i.J=-1;i.H=h;i.L=f;i.HH=false;
|
||||
i.P=d;i.DRT=false;i.ST=OrgNode.SF;i.TOC=j;i.DEPTH=g;i.F=null;i.CH=new Array();i.NAV="";
|
||||
i.BS=null;if(null!=i.P){i.P.addChild(this);i.hide();}var a=document.getElementById("text-"+i.I);
|
||||
if(null==a&&b){var c=b.substring(4);a=document.getElementById("text-"+c);}if(null!=a){i.F=a;
|
||||
}i.iTF=new Object();i.iTF["#"+i.I]=2;OrgNode.fTI(i.iTF,i.H,1);OrgNode.fTI(i.iTF,i.F,3);
|
||||
}OrgNode.SF=0;OrgNode.SH=1;OrgNode.SU=2;OrgNode.fTI=function(f,c,e){if(c){var b=c.getElementsByTagName("a");
|
||||
if(b){for(var d=0;d<b.length;++d){var g=b[d].getAttribute("id");if(g){f["#"+g]=e;
|
||||
}else{g=b[d].getAttribute("name");if(g){f["#"+g]=e;}}}}}};OrgNode.hE=function(a){if(a&&a.style){a.style.display="none";
|
||||
a.style.visibility="hidden";}};OrgNode.sE=function(a){if(a&&a.style){a.style.display="block";
|
||||
a.style.visibility="visible";}};OrgNode.uhE=function(a){a.style.display="";a.style.visibility="";
|
||||
};OrgNode.isHidden=function(a){if(a.style.display=="none"||a.style.visibility=="hidden"){return true;
|
||||
}return false;};OrgNode.toggleElement=function(a){if(a.style.display=="none"){a.style.display="block";
|
||||
a.style.visibility="visible";}else{a.style.display="none";a.style.visibility="hidden";
|
||||
}};OrgNode.textNodeToIdx=function(b,c){while(b.nodeType!=1||-1==b.attributes.id.value.indexOf("outline-container-")){b=b.parentNode;
|
||||
}var a=b.attributes.id.value.substr(18);return OrgNode.idxForBaseId(a,c);};OrgNode.idxForBaseId=function(b,d){if(d.I==b){return d;
|
||||
}for(var a=0;a<d.CH.length;++a){var c=OrgNode.idxForBaseId(idx,d.CH[a]);if(null!=c){return c;
|
||||
}}return null;};OrgNode.prototype.addChild=function(a){this.CH.push(a);return this.P;
|
||||
};OrgNode.prototype.hide=function(){OrgNode.hE(this.D);if(this.P){this.P.hide();}};
|
||||
OrgNode.prototype.show=function(){OrgNode.sE(this.D);if(this.DEPTH>2){this.P.show();
|
||||
}};OrgNode.prototype.sAC=function(){for(var a=0;a<this.CH.length;++a){this.CH[a].sAC();
|
||||
}this.show();};OrgNode.prototype.hAC=function(){for(var a=0;a<this.CH.length;++a){this.CH[a].hAC();
|
||||
}this.hide();};OrgNode.prototype.setLinkClass=function(a){if(this.TOC){if(a){this.TOC.className="current";
|
||||
}else{this.TOC.className="visited_after_load";}}};OrgNode.prototype.fold=function(b){if(this.P){this.P.DRT=true;
|
||||
}if(this.DRT){this.DRT=false;this.ST=OrgNode.SU;}if(null!=this.F){if(this.ST==OrgNode.SF){if(this.CH.length){this.ST=OrgNode.SH;
|
||||
OrgNode.hE(this.F);for(var a=0;a<this.CH.length;++a){this.CH[a].sSt(OrgNode.SH);}}else{if(!b){this.ST=OrgNode.SU;
|
||||
OrgNode.sE(this.F);}}}else{if(this.ST==OrgNode.SH){this.ST=OrgNode.SU;OrgNode.sE(this.F);
|
||||
for(var a=0;a<this.CH.length;++a){this.CH[a].sSt(OrgNode.SU);}}else{this.ST=OrgNode.SF;
|
||||
OrgNode.hE(this.F);for(var a=0;a<this.CH.length;++a){this.CH[a].sSt(OrgNode.SF);}}}}};
|
||||
OrgNode.prototype.sSt=function(c){var b=this;for(var a=0;a<b.CH.length;++a){b.CH[a].sSt(c);
|
||||
}switch(c){case OrgNode.SF:OrgNode.hE(b.F);OrgNode.hE(b.D);break;case OrgNode.SH:OrgNode.hE(b.F);
|
||||
OrgNode.sE(b.D);break;default:OrgNode.sE(b.F);OrgNode.sE(b.D);}b.ST=c;};var org_html_manager={MOUSE_HINT:0,B:null,PLAIN_VIEW:0,CONTENT_VIEW:1,ALL_VIEW:2,INFO_VIEW:3,SLIDE_VIEW:4,VIEW:this.CONTENT_VIEW,LOCAL_TOC:false,LINK_HOME:0,LINK_UP:0,LINKS:"",RUN_MAX:1200,RUN_INTERVAL:100,HIDE_TOC:false,TOC_DEPTH:0,STARTUP_MESSAGE:0,P:null,BU:document.URL,Q:"",R:null,N:null,T:null,IT:false,LOAD_CHECK:null,W:null,S:new Array(),REGEX:/(#)(.*$)/,SIDX:/(^#)(sec-\d+([._]\d+)*$)/,UNTAGX:/<[^>]+>/i,ORGTAGX:/^(.*)<span\s+class=[\'\"]tag[\'\"]>(<span[^>]+>[^<]+<\/span>)+<\/span>/i,TRIMMER:/^(\s*)([^\s].*)(\s*)$/,TOC:null,RUNS:0,H:new Array(50),HI:0,SKIP_H:false,FIXED_TOC:false,C:null,CI:null,CL:null,CO:"50px",OCCUR:"",SCX:"",SC_HLX:new RegExp('(<span class="org-info-js_search-highlight">)([^<]*?)(</span>)',"gi"),Mg:0,MgI:1,MgT:2,Hg:false,Rg:false,RC:"",RC_NULL:"_0",RC_H:"_1",RC_O:"_2",RC_P:"_03",LVM:0,TAB_INDEX:1000,SHO:false,TAGS:{},ST:new Array(),TAGS_INDEX:null,CTO:null,SN_MAP:{},TL:null,HOOKS:{run_hooks:false,onShowSection:[],onReady:[]},setup:function(){var d=this;
|
||||
if(window.orgInfoHooks){for(var c in orgInfoHooks){d.HOOKS[c]=orgInfoHooks[c];}d.HOOKS.run_hooks=false;
|
||||
}if(location.search){var e=location.search.substring(1).split("&");for(var c=0;c<e.length;
|
||||
++c){var f=e[c].indexOf("=");if(-1!=f){var b=e[c].substring(f+1);var a=e[c].substring(0,f);
|
||||
switch(a){case"TOC":case"TOC_DEPTH":case"MOUSE_HINT":case"HELP":case"VIEW":case"HIDE_TOC":case"LOCAL_TOC":case"OCCUR":d.set(a,decodeURIComponent(b));
|
||||
break;default:break;}}}}d.VIEW=d.VIEW?d.VIEW:d.PLAIN_VIEW;d.VIEW_BUTTONS=(d.VIEW_BUTTONS&&d.VIEW_BUTTONS!="0")?true:false;
|
||||
d.STARTUP_MESSAGE=(d.STARTUP_MESSAGE&&d.STARTUP_MESSAGE!="0")?true:false;d.LOCAL_TOC=(d.LOCAL_TOC&&d.LOCAL_TOC!="0")?d.LOCAL_TOC:false;
|
||||
d.HIDE_TOC=(d.TOC&&d.TOC!="0")?false:true;d.IT=(d.IT&&d.IT!="title_above")?false:true;
|
||||
if(d.FIXED_TOC&&d.FIXED_TOC!="0"){d.FIXED_TOC=true;d.HIDE_TOC=false;}else{d.FIXED_TOC=false;
|
||||
}d.LINKS+=((d.LINK_UP&&d.LINK_UP!=document.URL)?'<a href="'+d.LINK_UP+'">Up</a> / ':"")+((d.LINK_HOME&&d.LINK_HOME!=document.URL)?'<a href="'+d.LINK_HOME+'">HOME</a> / ':"")+'<a href="javascript:org_html_manager.showHelp();">HELP</a> / ';
|
||||
d.LOAD_CHECK=window.setTimeout("OrgHtmlManagerLoadCheck()",50);},trim:function(a){var b=this.TRIMMER.exec(a);
|
||||
return RegExp.$2;},rT:function(a){if(a){while(a.match(this.UNTAGX)){a=a.substr(0,a.indexOf("<"))+a.substr(a.indexOf(">")+1);
|
||||
}}return a;},rOT:function(a){if(a.match(this.ORGTAGX)){var b=this.ORGTAGX.exec(a);
|
||||
return b[1];}return a;},init:function(){var m=this;m.RUNS++;m.B=document.getElementById("content");
|
||||
if(null==m.B){if(5>m.RUNS){m.LOAD_CHECK=window.setTimeout("OrgHtmlManagerLoadCheck()",m.RUN_INTERVAL);
|
||||
return;}else{m.B=document.getElementsByTagName("body")[0];}}if(!m.W){m.W=document.createElement("div");
|
||||
m.W.style.marginBottom="40px";m.W.id="org-info-js-window";}var l=document.getElementById("table-of-contents");
|
||||
if(!m.initFromTOC()){if(m.RUNS<m.RUN_MAX){m.LOAD_CHECK=window.setTimeout("OrgHtmlManagerLoadCheck()",m.RUN_INTERVAL);
|
||||
return;}}var d=0;var f=false;if(""!=location.hash){m.BU=m.BU.substring(0,m.BU.indexOf("#"));
|
||||
for(var e=0;e<m.S.length;++e){if(m.S[e].iTF[location.hash]){d=e;f=1;break;}}}if(""!=location.search){m.Q=m.BU.substring(m.BU.indexOf("?"));
|
||||
m.BU=m.BU.substring(0,m.BU.indexOf("?"));}m.convertLinks();var j=document.getElementById("postamble");
|
||||
if(j){m.P=j;}var h=m.B;var c=h.firstChild;if(3==c.nodeType){var g=c.cloneNode(true);
|
||||
var a=document.createElement("p");a.id="text-before-first-headline";a.appendChild(g);
|
||||
h.replaceChild(a,c);}m.C=document.createElement("div");m.C.innerHTML='<form action="" style="margin:0px;padding:0px;" onsubmit="org_html_manager.eRC(); return false;"><table id="org-info-js_console" style="width:100%;margin:0px 0px 0px 0px;border-style:none;" cellpadding="0" cellspacing="0" summary="minibuffer"><tbody><tr><td id="org-info-js_console-icon" style="padding:0px 0px 0px 0px;border-style:none;"> </td><td style="width:100%;vertical-align:middle;padding:0px 0px 0px 0px;border-style:none;"><table style="width:100%;margin:0px 0px 0px 0px;border-style:none;" cellpadding="0" cellspacing="2"><tbody><tr><td id="org-info-js_console-label" style="white-space:nowrap;padding:0px 0px 0px 0px;border-style:none;"></td></tr><tr><td style="width:100%;vertical-align:middle;padding:0px 0px 0px 0px;border-style:none;"><input type="text" id="org-info-js_console-input" onkeydown="org_html_manager.getKey();" onclick="this.select();" maxlength="150" style="width:100%;padding:0px;margin:0px 0px 0px 0px;border-style:none;" value=""/></td></tr></tbody></table></td><td style="padding:0px 0px 0px 0px;border-style:none;"> </td></tr></tbody></table></form>';
|
||||
m.C.style.position="relative";m.C.style.marginTop="-"+m.CO;m.C.style.top="-"+m.CO;
|
||||
m.C.style.left="0px";m.C.style.width="100%";m.C.style.height="40px";m.C.style.overflow="hidden";
|
||||
m.C.style.verticalAlign="middle";m.C.style.zIndex="9";m.C.style.border="0px solid #cccccc";
|
||||
m.C.id="org-info-js_console-container";m.B.insertBefore(m.C,m.B.firstChild);m.Mg=false;
|
||||
m.CL=document.getElementById("org-info-js_console-label");m.CI=document.getElementById("org-info-js_console-input");
|
||||
document.onkeypress=OrgHtmlManagerKeyEvent;if(m.VIEW==m.INFO_VIEW){m.iV(d);m.ss(d);
|
||||
window.setTimeout(function(){window.scrollTo(0,0);},100);}else{if(m.VIEW==m.SLIDE_VIEW){m.sV(d);
|
||||
m.ss(d);}else{var k=m.VIEW;m.pV(d,1);m.R.DRT=true;m.R_STATE=OrgNode.SU;m.tG();if(k>m.PLAIN_VIEW){m.tG();
|
||||
}if(k==m.ALL_VIEW){m.tG();}if(f){m.ss(d);}}}if(""!=m.OCCUR){m.CI.value=m.OCCUR;m.RC="o";
|
||||
m.eRC();}if(m.STARTUP_MESSAGE){m.warn("This page uses org-info.js. Press '?' for more information.",true);
|
||||
}m.HOOKS.run_hooks=true;m.runHooks("onReady",this.N);},initFromTOC:function(){var k=this;
|
||||
if(k.RUNS==1||!k.R){var b=document.getElementById("table-of-contents");if(null!=b){var m=null;
|
||||
var d=0;for(d;m==null&&d<7;++d){m=b.getElementsByTagName("h"+d)[0];}m.onclick=function(){org_html_manager.fold(0);
|
||||
};m.style.cursor="pointer";if(k.MOUSE_HINT){m.onmouseover=function(){org_html_manager.hH(0);
|
||||
};m.onmouseout=function(){org_html_manager.unhH(0);};}if(k.FIXED_TOC){m.setAttribute("onclick","org_html_manager.tG();");
|
||||
k.R=new OrgNode(null,k.B.getElementsByTagName("h1")[0],"javascript:org_html_manager.go(0);",0,null);
|
||||
k.TOC=new OrgNode(b,m,"javascript:org_html_manager.go(0);",d,null);k.N=k.R;}else{k.R=new OrgNode(null,k.B.getElementsByTagName("h1")[0],"javascript:org_html_manager.go(0);",0,null);
|
||||
if(k.HIDE_TOC){k.TOC=new OrgNode(b,"","javascript:org_html_manager.go(0);",d,null);
|
||||
k.N=k.R;OrgNode.hE(b);}else{k.TOC=new OrgNode(b,m,"javascript:org_html_manager.go(0);",d,k.R);
|
||||
k.TOC.J=0;k.N=k.TOC;k.S.push(k.TOC);}}if(k.TOC){k.TOC.F=document.getElementById("text-table-of-contents");
|
||||
}}else{return false;}}var j=k.TOC.F.getElementsByTagName("ul")[0];if(!k.ulToOutlines(j)){return false;
|
||||
}var h=document.getElementById("footnotes");if(h){var a=null;var f=h.childNodes;for(var d=0;
|
||||
d<f.length;++d){if("footnotes"==f[d].className){a=f[d];break;}}var e=k.S.length;a.onclick=function(){org_html_manager.fold(""+e);
|
||||
};a.style.cursor="pointer";if(k.MOUSE_HINT){a.onmouseover=function(){org_html_manager.hH(""+e);
|
||||
};a.onmouseout=function(){org_html_manager.unhH(""+e);};}var g="javascript:org_html_manager.go("+e+")";
|
||||
var l=new OrgNode(h,a,g,1,k.R,"footnotes");k.S.push(l);}if(k.TOC_DEPTH){k.cutToc(j,1);
|
||||
}k.T=k.B.getElementsByTagName("h1")[0];if(k.IT&&!k.FIXED_TOC&&k.VIEW!=k.SLIDE_VIEW){k.IT=k.T.cloneNode(true);
|
||||
k.S[0].D.insertBefore(k.IT,k.S[0].D.firstChild);OrgNode.hE(k.T);}k.build();k.N=k.S[0];
|
||||
k.B.insertBefore(k.W,k.N.D);return true;},ulToOutlines:function(b){if(b.hasChildNodes()&&!b.scanned_for_org){for(var a=0;
|
||||
a<b.childNodes.length;++a){if(false==this.liToOutlines(b.childNodes[a])){return false;
|
||||
}}b.scanned_for_org=1;}return true;},liToOutlines:function(b){if(!b.scanned_for_org){for(var d=0;
|
||||
d<b.childNodes.length;++d){var e=b.childNodes[d];switch(e.nodeName){case"A":var a=this.mkNodeFromHref(e);
|
||||
if(false==a){return false;}else{e.href=a;e.tabIndex=this.TAB_INDEX;e.onfocus=function(){org_html_manager.TL=this;
|
||||
void 0;};if(null==this.TL){this.TL=e;}this.TAB_INDEX++;}break;case"UL":return this.ulToOutlines(e);
|
||||
break;}}b.scanned_for_org=1;}return true;},cutToc:function(e,f){f++;if(e.hasChildNodes()){for(var d=0;
|
||||
d<e.childNodes.length;++d){var a=e.childNodes[d];for(var b=0;b<a.childNodes.length;
|
||||
++b){var g=a.childNodes[b];if(g.nodeName=="UL"){if(f>this.TOC_DEPTH){a.removeChild(g);
|
||||
}else{this.cutToc(g,f);}}}}}},mkNodeFromHref:function(g){s=g.href;if(s.match(this.REGEX)){var k=this.REGEX.exec(s);
|
||||
var c=k[2];var l=document.getElementById(c);if(null==l){return(false);}var a=l.parentNode;
|
||||
var m=this.S.length;var f=a.className.substr(8);l.onclick=function(){org_html_manager.fold(""+m);
|
||||
};l.style.cursor="pointer";if(this.MOUSE_HINT){l.onmouseover=function(){org_html_manager.hH(""+m);
|
||||
};l.onmouseout=function(){org_html_manager.unhH(""+m);};}var o="javascript:org_html_manager.go("+m+")";
|
||||
if(f>this.N.DEPTH){this.N=new OrgNode(a,l,o,f,this.N,c,g);}else{if(f==2){this.N=new OrgNode(a,l,o,f,this.R,c,g);
|
||||
}else{var b=this.N;while(b.DEPTH>f){b=b.P;}this.N=new OrgNode(a,l,o,f,b.P,c,g);}}this.S.push(this.N);
|
||||
var n=l.getElementsByTagName("span");if(n){for(var e=0;e<n.length;++e){if(n[e].className=="tag"){var r=n[e].innerHTML.split(" ");
|
||||
for(var d=0;d<r.length;++d){var q=this.rT(r[d]);if(!this.TAGS[q]){this.TAGS[q]=new Array();
|
||||
this.ST.push(q);}this.TAGS[q].push(m);}}else{if(n[e].className.match(this.SECNUMX)){this.SN_MAP[this.trim(n[e].innerHTML)]=this.N;
|
||||
}}}}this.N.hide();return(o);}return(s);},build:function(){var f=this.T.innerHTML;
|
||||
var e=0;for(var d=0;d<this.S.length;++d){this.S[d].J=d;var c='<table class="org-info-js_info-navigation" width="100%" border="0" style="border-bottom:1px solid black;"><tr><td colspan="3" style="text-align:left;border-style:none;vertical-align:bottom;"><span style="float:left;display:inline;text-align:left;">Top: <a accesskey="t" href="javascript:org_html_manager.go(0);">'+f+'</a></span><span style="float:right;display:inline;text-align:right;font-size:70%;">'+this.LINKS+'<a accesskey="m" href="javascript:org_html_manager.toggleView('+d+');">toggle view</a></span></td></tr><tr><td style="text-align:left;border-style:none;vertical-align:bottom;width:22%">';
|
||||
if(d>0){c+='<a accesskey="p" href="'+this.S[d-1].L+'" title="Go to: '+this.rT(this.S[d-1].H.innerHTML)+'">Previous</a> | ';
|
||||
}else{c+="Previous | ";}if(d<this.S.length-1){c+='<a accesskey="n" href="'+this.S[d+1].L+'" title="Go to: '+this.rT(this.S[d+1].H.innerHTML)+'">Next</a>';
|
||||
}else{c+="Next";}c+='</td><td style="text-align:center;vertical-align:bottom;border-style:none;width:56%;">';
|
||||
if(d>0&&this.S[d].P.P){c+='<a href="'+this.S[d].P.L+'" title="Go to: '+this.rT(this.S[d].P.H.innerHTML)+'"><span style="font-variant:small-caps;font-style:italic;">'+this.S[d].P.H.innerHTML+"</span></a>";
|
||||
}else{c+='<span style="font-variant:small-caps;font-style:italic;">'+this.S[d].H.innerHTML+"</span>";
|
||||
}c+='</td><td style="text-align:right;vertical-align:bottom;border-style:none;width:22%">';
|
||||
c+=(d+1)+"</td></tr></table>";this.S[d].BS=document.createElement("div");this.S[d].BS.innerHTML='<div class="org-info-js_header-navigation" style="display:inline;float:right;text-align:right;font-size:70%;font-weight:normal;">'+this.LINKS+'<a accesskey="m" href="javascript:org_html_manager.toggleView('+d+');">toggle view</a></div>';
|
||||
if(this.S[d].F){this.S[d].D.insertBefore(this.S[d].BS,this.S[d].H);}else{if(this.S[d].D.hasChildNodes()){this.S[d].D.insertBefore(this.S[d].BS,this.S[d].D.firstChild);
|
||||
}}if(!this.VIEW_BUTTONS){OrgNode.hE(this.S[d].BS);}this.S[d].NAV=c;if(0<this.S[d].CH.length&&this.LOCAL_TOC){var a=document.createElement("div");
|
||||
a.className="org-info-js_local-toc";c="Contents:<br /><ul>";for(var b=0;b<this.S[d].CH.length;
|
||||
++b){c+='<li><a href="'+this.S[d].CH[b].L+'">'+this.rT(this.rOT(this.S[d].CH[b].H.innerHTML))+"</a></li>";
|
||||
}c+="</ul>";a.innerHTML=c;if("above"==this.LOCAL_TOC){if(this.S[d].F){this.S[d].F.insertBefore(a,this.S[d].F.firstChild);
|
||||
}else{this.S[d].D.insertBefore(a,this.S[d].D.getElementsByTagName("h"+this.S[d].DEPTH)[0].nextSibling);
|
||||
}}else{if(this.S[d].F){this.S[d].F.appendChild(a);}else{this.S[d].D.appendChild(a);
|
||||
}}}}this.ST.sort();},set:function(eval_key,eval_val){if("VIEW"==eval_key){var pos=eval_val.indexOf("_");
|
||||
if(-1!=pos){this.IT=eval_val.substr(pos+1);eval_val=eval_val.substr(0,pos);}var overview=this.PLAIN_VIEW;
|
||||
var content=this.CONTENT_VIEW;var showall=this.ALL_VIEW;var info=this.INFO_VIEW;var info_title_above=this.INFO_VIEW;
|
||||
var slide=this.SLIDE_VIEW;eval("this."+eval_key+"="+eval_val+";");}else{if("HELP"==eval_key){eval("this.STARTUP_MESSAGE="+eval_val+";");
|
||||
}else{if(eval_val){eval("this."+eval_key+"='"+eval_val+"';");}else{eval("this."+eval_key+"=0;");
|
||||
}}}},convertLinks:function(){var f=(this.HIDE_TOC?0:1);var e;var a=this.S.length-1;
|
||||
var d=document.getElementsByTagName("a");for(e=0;e<d.length;++e){var c=d[e].href.replace(this.BU,"");
|
||||
for(var b=0;b<this.S.length;++b){if(this.S[b].iTF[c]){d[e].href="javascript:org_html_manager.go("+b+")";
|
||||
break;}}}},ss:function(d){var b=this;var f=parseInt(d);var c=b.N;var e="onShowSection";
|
||||
if(b.HIDE_TOC&&b.N==b.TOC&&!b.FIXED_TOC){OrgNode.hE(b.TOC.D);if(b.PLAIN_VIEW==b.VIEW){b.R.sAC();
|
||||
for(var a=0;a<b.R.CH.length;++a){b.R.CH[a].ST=OrgNode.SU;b.R.CH[a].fold();}}}if("?/toc/?"!=d&&null!=b.TL){b.TL.blur();
|
||||
}if("?/toc/?"==d||(!isNaN(f)&&b.S[f])){if("?/toc/?"==d&&b.HIDE_TOC){e="onShowToc";
|
||||
b.N=b.TOC;b.R.hAC();if(b.INFO_VIEW==b.VIEW){b.W.innerHTML=b.N.D.innerHTML;}else{b.N.sSt(OrgNode.SU);
|
||||
}window.scrollTo(0,0);}else{b.N=b.S[f];if(b.SLIDE_VIEW==b.VIEW||b.INFO_VIEW==b.VIEW){OrgNode.hE(b.N.BS);
|
||||
b.N.sSt(OrgNode.SU);for(var a=0;a<b.N.CH.length;++a){b.N.CH[a].hide();}if(b.SLIDE_VIEW==b.VIEW){b.W.innerHTML=b.N.D.innerHTML;
|
||||
}else{b.W.innerHTML=b.N.NAV+b.N.D.innerHTML;}b.N.hide();if(!b.FIXED_TOC){OrgNode.hE(document.body);
|
||||
}if(c.J!=b.N.J){if("?/toc/?"!=d){window.location.replace(b.BU+b.Q+b.dT());}}if(!b.FIXED_TOC){OrgNode.sE(document.body);
|
||||
}}else{if(!b.VIEW_BUTTONS){OrgNode.hE(c.BS);}OrgNode.sE(b.N.BS);b.N.sSt(OrgNode.UNFOLDED);
|
||||
b.N.show();if(c.J!=b.N.J){window.location.replace(b.BU+b.Q+b.dT());}if(b.N.J==0){window.scrollTo(0,0);
|
||||
}else{b.N.D.scrollIntoView(true);}}}}c.setLinkClass();b.N.setLinkClass(true);b.runHooks(e,{last:c,current:b.N});
|
||||
},pV:function(d,a){var c=this;document.onclick=null;document.ondblclick=null;c.VIEW=c.PLAIN_VIEW;
|
||||
OrgNode.hE(c.W);if(c.IT){OrgNode.hE(c.IT);}OrgNode.sE(c.T);if(c.W.firstChild){c.W.removeChild(c.W.firstChild);
|
||||
}c.R.sAC();for(var b=0;b<c.R.CH.length;++b){c.R.CH[b].ST=OrgNode.SU;c.R.CH[b].fold();
|
||||
}if(!a){c.ss(d);}if(c.P){OrgNode.sE(c.P);}if(c.N.J==0){window.scrollTo(0,0);}else{c.N.D.scrollIntoView(true);
|
||||
}},iV:function(c,a){var b=this;document.onclick=null;document.ondblclick=null;b.VIEW=b.INFO_VIEW;
|
||||
b.unhH(b.N.J);if(b.IT&&!b.FIXED_TOC){OrgNode.sE(b.IT);OrgNode.hE(b.T);}OrgNode.sE(b.W);
|
||||
b.R.hAC();if(b.TOC&&!b.FIXED_TOC){OrgNode.hE(b.TOC.D);}if(b.P){OrgNode.sE(b.P);}if(!a){b.ss(c);
|
||||
}window.scrollTo(0,0);},sV:function(c,a){var b=this;b.VIEW=b.SLIDE_VIEW;b.unhH(b.N.J);
|
||||
OrgNode.hE(b.T);if(b.IT){OrgNode.hE(b.IT);}if(b.TOC){OrgNode.hE(b.TOC.D);}OrgNode.sE(b.T);
|
||||
OrgNode.sE(b.W);b.R.hAC();OrgNode.hE(b.TOC.D);if(b.P){OrgNode.hE(b.P);}b.adjustSlide(c);
|
||||
if(!a){b.ss(c);}},adjustSlide:function(f,g){var k=true;var e=true;var d=false;if(f>this.N.J){d=true;
|
||||
}if(null==g){d=true;}if(d){for(var a=this.S[f].F.firstChild;null!=a;a=a.nextSibling){if("UL"==a.nodeName){var j=a.getElementsByTagName("li");
|
||||
for(var c=1;c<j.length;++c){var b=j[c];OrgNode.hE(b);k=false;}}}}else{var h=this.W.getElementsByTagName("ul");
|
||||
for(var a=0;a<h.length;++a){var j=h[a].getElementsByTagName("li");for(var c=1;c<j.length;
|
||||
++c){var b=j[c];if(g>0){if(OrgNode.isHidden(b)){OrgNode.uhE(b);if(c<(j.length-1)){k=false;
|
||||
}if(0<c){e=false;}break;}}else{if(!OrgNode.isHidden(b)){if(1<c){e=false;OrgNode.hE(j[c-1]);
|
||||
break;}}}}}}if(k){document.onclick=function(){org_html_manager.sCk("org_html_manager.nextSection(org_html_manager.N.J + 1)");
|
||||
};}else{document.onclick=function(){org_html_manager.sCk("org_html_manager.adjustSlide(org_html_manager.N.J, +1)");
|
||||
};}if(e){document.ondblclick=function(){org_html_manager.sCk("org_html_manager.previousSection()");
|
||||
};}else{document.ondblclick=function(){org_html_manager.sCk("org_html_manager.adjustSlide("+this.N.J+", -1)");
|
||||
};}},toggleView:function(b){var a=this;a.Q="";a.rW();if(a.VIEW==a.INFO_VIEW){a.pV(b);
|
||||
}else{a.iV(b);}},fold:function(b){var a=this;a.rW();var c=parseInt(b);a.S[c].fold();
|
||||
if(!a.VIEW_BUTTONS){OrgNode.hE(a.N.BS);}a.N=a.S[c];OrgNode.sE(a.N.BS);},tG:function(){var b=this;
|
||||
if(b.R.DRT){b.R.ST=OrgNode.SU;}if(OrgNode.SU==b.R.ST){for(var a=0;a<b.R.CH.length;
|
||||
++a){b.R.CH[a].ST=OrgNode.SU;b.R.CH[a].fold(true);}b.R.ST=OrgNode.SU;b.R.ST=OrgNode.SF;
|
||||
}else{if(OrgNode.SF==b.R.ST){for(var a=0;a<b.R.CH.length;++a){b.R.CH[a].fold(true);
|
||||
}b.R.ST=OrgNode.SH;}else{for(var a=0;a<b.R.CH.length;++a){b.R.CH[a].fold();}b.R.ST=OrgNode.SU;
|
||||
}}b.R.DRT=false;},executeClick:function(func){var t=this;if(t.Rg){t.eR();t.hC();}else{if(t.Mg){t.rW();
|
||||
}}eval(func);if(null!=t.CTO){t.CTO=null;}},sCk:function(b,a){if(null==a){a=250;}if(null==this.CTO){this.CTO=window.setTimeout("org_html_manager.executeClick("+b+")",a);
|
||||
}else{window.clearTimeout(this.CTO);this.CTO=null;}},nextSection:function(){var a=this;
|
||||
var b=a.N.J+1;if(b<a.S.length){a.go(b);}else{a.warn("Already last section.");}},previousSection:function(){var b=this;
|
||||
var a=b.N.J;if(a>0){b.go(a-1);}else{b.warn("Already first section.");}},go:function(b){var a=this;
|
||||
if(a.Rg){a.eR();a.hC();}else{if(a.Mg){a.rW();}}if(a.VIEW==a.SLIDE_VIEW){a.adjustSlide(b);
|
||||
}a.puH(b,a.N.J);a.ss(b);},puH:function(c,a){var b=this;if(!b.SKIP_H){b.H[b.HI]=new Array(c,a);
|
||||
b.HI=(b.HI+1)%50;}b.SKIP_H=false;b.CI.value="";},poH:function(c){var a=this;if(c){if(a.H[a.HI]){var b=parseInt(a.H[a.HI][0]);
|
||||
if(!isNaN(b)||"?/toc/?"==a.H[a.HI][0]){a.ss(a.H[a.HI][0]);a.CI.value="";}else{a.SKIP_H=true;
|
||||
a.CI.value=a.H[a.HI][0];a.getKey();}a.HI=(a.HI+1)%50;a.HBO=0;}else{if(a.HFO&&history.length){history.forward();
|
||||
}else{a.HFO=1;a.warn("History: No where to foreward go from here. Any key and `B' to move to next file in history.");
|
||||
}}}else{if(a.H[a.HI-1]){a.HI=a.HI==0?49:a.HI-1;var b=parseInt(a.H[a.HI][1]);if(!isNaN(b)||"?/toc/?"==a.H[a.HI][1]){a.ss(a.H[a.HI][1]);
|
||||
a.CI.value="";}else{a.SKIP_H=true;a.CI.value=a.H[a.HI][1];a.getKey();}a.HFO=0;}else{if(a.HBO&&history.length){history.back();
|
||||
}else{a.HBO=1;a.warn("History: No where to back go from here. Any key and `b' to move to previous file in history.");
|
||||
}}}},warn:function(c,d,b){var a=this;if(null==b){b="";}a.CI.value=b;if(!d){a.CL.style.color="red";
|
||||
}a.CL.innerHTML="<span style='float:left;'>"+c+"</span><span style='float:right;color:#aaaaaa;font-weight:normal;'>(press any key to proceed)</span>";
|
||||
a.sC();window.setTimeout(function(){org_html_manager.CI.value=b;},50);},sR:function(e,b,d,a){var c=this;
|
||||
if(null==d){d="";}if(null==a){a="";}c.RC=e;c.Rg=true;c.CL.innerHTML="<span style='float:left;'>"+b+"</span><span style='float:right;color:#aaaaaa;font-weight:normal;'>("+a+"RET to close)</span>";
|
||||
c.sC();document.onkeypress=null;c.CI.focus();c.CI.onblur=function(){org_html_manager.CI.focus();
|
||||
};window.setTimeout(function(){org_html_manager.CI.value=d;},50);},eR:function(c,a){var b=this;
|
||||
b.Rg=false;b.RC="";b.CI.onblur=null;b.CI.blur();document.onkeypress=OrgHtmlManagerKeyEvent;
|
||||
},rW:function(){var a=this;a.CL.style.color="#333333";a.hC();},sC:function(){var a=this;
|
||||
if(!a.Mg){if(a.VIEW==a.PLAIN_VIEW){a.B.removeChild(a.B.firstChild);a.N.D.insertBefore(a.C,a.N.D.firstChild);
|
||||
a.N.D.scrollIntoView(true);a.Mg=a.MgI;}else{a.Mg=a.MgT;window.scrollTo(0,0);}a.C.style.marginTop="0px";
|
||||
a.C.style.top="0px";}},hC:function(){var a=this;if(a.Mg){a.C.style.marginTop="-"+a.CO;
|
||||
a.C.style.top="-"+a.CO;a.CL.innerHTML="";a.CI.value="";if(a.MgI==a.Mg){a.N.D.removeChild(a.N.D.firstChild);
|
||||
a.B.insertBefore(a.C,a.B.firstChild);if(a.N.J!=0){a.N.D.scrollIntoView();}}a.Mg=false;
|
||||
}},getKey:function(){var b=this;var c=b.CI.value;if(0==c.length){if(b.Hg){b.showHelp();
|
||||
return;}if(b.Mg&&!b.Rg){b.rW();}return;}if(b.Mg&&!b.Rg){b.rW();return;}else{if(b.Hg){b.showHelp();
|
||||
b.CI.value="";return;}else{if(b.Rg){return;}}}b.CI.value="";b.CI.blur();if(b.HIDE_TOC&&b.TOC==b.N&&"v"!=c&&"V"!=c&&"\t"!=c){c="b";
|
||||
}else{if("\t"==c){return true;}else{c=b.trim(c);}}if(1==c.length){if("b"==c){b.poH();
|
||||
}else{if("B"==c){b.poH(true);}else{if("c"==c){b.rSH();if(b.VIEW==b.INFO_VIEW||b.VIEW==b.SLIDE_VIEW){b.ss(b.N.J);
|
||||
}}else{if("i"==c){if(!b.FIXED_TOC){if(b.HIDE_TOC){b.go("?/toc/?");}else{if(0!=b.N.J){b.go(0);
|
||||
}}}if(null!=b.TL){b.TL.focus();}}else{if("m"==c){b.toggleView(b.N.J);return;}else{if("x"==c){b.sV(b.N.J);
|
||||
}else{if("n"==c){if(b.N.ST==OrgNode.SF&&b.VIEW==b.PLAIN_VIEW){b.ss(b.N.J);}else{if(b.N.J<b.S.length-1){b.go(b.N.J+1);
|
||||
}else{b.warn("Already last section.");return;}}}else{if("N"==c){if(b.N.J<b.S.length-1){var e=b.N.DEPTH;
|
||||
var a=b.N.J+1;while(a<b.S.length-1&&b.S[a].DEPTH>=e){if(b.S[a].DEPTH==e){b.go(a);
|
||||
return;}++a;}}b.warn("No next sibling.");return;}else{if("p"==c){if(b.N.J>0){b.go(b.N.J-1);
|
||||
}else{b.warn("Already first section.");return;}}else{if("P"==c){if(b.N.J>0){var e=b.N.DEPTH;
|
||||
var a=b.N.J-1;while(a>=0&&b.S[a].DEPTH>=e){if(b.S[a].DEPTH==e){b.go(a);return;}--a;
|
||||
}}b.warn("No previous sibling.");}else{if("q"==c){if(window.confirm("Really close this file?")){window.close();
|
||||
}}else{if("<"==c||"t"==c){if(0!=b.N.J){b.go(0);}else{window.scrollTo(0,0);}}else{if(">"==c||"E"==c||"e"==c){if((b.S.length-1)!=b.N.J){b.go(b.S.length-1);
|
||||
}else{b.S[b.S.length-1].D.scrollIntoView(true);}}else{if("v"==c){if(window.innerHeight){window.scrollBy(0,window.innerHeight-30);
|
||||
}else{if(document.documentElement.clientHeight){window.scrollBy(0,document.documentElement.clientHeight-30);
|
||||
}else{window.scrollBy(0,document.body.clientHeight-30);}}}else{if("V"==c){if(window.innerHeight){window.scrollBy(0,-(window.innerHeight-30));
|
||||
}else{if(document.documentElement.clientHeight){window.scrollBy(0,-(document.documentElement.clientHeight-30));
|
||||
}else{window.scrollBy(0,-(document.body.clientHeight-30));}}}else{if("u"==c){if(b.N.P!=b.R){b.N=b.N.P;
|
||||
b.ss(b.N.J);}}else{if("W"==c){b.pV(b.N.J);b.R.DRT=true;b.R_STATE=OrgNode.SU;b.tG();
|
||||
b.tG();b.tG();window.print();}else{if("f"==c){if(b.VIEW!=b.INFO_VIEW){b.N.fold();
|
||||
b.N.D.scrollIntoView(true);}}else{if("F"==c){if(b.VIEW!=b.INFO_VIEW){b.tG();b.N.D.scrollIntoView(true);
|
||||
}}else{if("?"==c||"¿"==c){b.showHelp();}else{if("C"==c){if(b.ST.length){b.showTagsIndex();
|
||||
}else{b.warn("No Tags found.");}}else{if("H"==c&&b.LINK_HOME){window.document.location.href=b.LINK_HOME;
|
||||
}else{if("h"==c&&b.LINK_UP){window.document.location.href=b.LINK_UP;}else{if("l"==c){if(""!=b.OCCUR){b.sR(b.RC_H,"Choose HTML-link type: 's' = section, 'o' = occur");
|
||||
}else{b.sR(c,"HTML-link:",'<a href="'+b.BU+b.dT()+'">'+document.title+", Sec. '"+b.rT(b.N.H.innerHTML)+"'</a>","C-c to copy, ");
|
||||
window.setTimeout(function(){org_html_manager.CI.select();},100);}return;}else{if("L"==c){if(""!=b.OCCUR){b.sR(b.RC_O,"Choose Org-link type: 's' = section, 'o' = occur");
|
||||
}else{b.sR(c,"Org-link:","[["+b.BU+b.dT()+"]["+document.title+", Sec. '"+b.rT(b.N.H.innerHTML)+"']]","C-c to copy, ");
|
||||
window.setTimeout(function(){org_html_manager.CI.select();},100);}return;}else{if("U"==c){if(""!=b.OCCUR){b.sR(b.RC_P,"Choose Org-link type: 's' = section, 'o' = occur");
|
||||
}else{b.sR(c,"Plain URL Link:",b.BU+b.dT(),"C-c to copy, ");window.setTimeout(function(){org_html_manager.CI.select();
|
||||
},100);}return;}else{if("g"==c){b.sR(c,"Enter section number:");return;}else{if("o"==c){if(""!=b.OCCUR){b.sR(c,"Occur:",b.OCCUR,"RET to use previous, DEL ");
|
||||
}else{b.sR(c,"Occur:",b.OCCUR);}window.setTimeout(function(){org_html_manager.CI.value=org_html_manager.OCCUR;
|
||||
org_html_manager.CI.select();},100);return;}else{if("s"==c){if(""!=b.OCCUR){b.sR(c,"Search forward:",b.OCCUR,"RET to use previous, DEL ");
|
||||
}else{b.sR(c,"Search forward:",b.OCCUR);}window.setTimeout(function(){org_html_manager.CI.value=org_html_manager.OCCUR;
|
||||
org_html_manager.CI.select();},100);return;}else{if("S"==c){if(""==b.OCCUR){c="s";
|
||||
b.sR(c,"Search forward:");}else{b.RC=c;b.eRC();}return;}else{if("r"==c){if(""!=b.OCCUR){b.sR(c,"Search backwards:",b.OCCUR,"RET to use previous, DEL ");
|
||||
}else{b.sR(c,"Search backwards:",b.OCCUR);}window.setTimeout(function(){org_html_manager.CI.value=org_html_manager.OCCUR;
|
||||
org_html_manager.CI.select();},100);return;}else{if("R"==c){if(""==b.OCCUR){c="r";
|
||||
b.sR(c,"Search backwards:");}else{b.RC=c;b.eRC();}return;}}}}}}}}}}}}}}}}}}}}}}}}}}}}}}}}}return;
|
||||
},eRC:function(){var j=this;var a=j.RC;var k=j.trim(j.CI.value);j.eR();if(""==a||""==k){j.hC();
|
||||
return;}if(a=="g"){var f=j.SN_MAP[k];if(null!=f){j.hC();j.go(f.J);return;}j.warn("Goto section: no such section.",false,k);
|
||||
return;}else{if(a=="s"){if(""==k){return false;}if(j.SHO){j.rSH();}var g=j.OCCUR;
|
||||
var e=0;if(k==j.OCCUR){e++;}j.OCCUR=k;j.mSR();for(var d=j.N.J+e;d<j.S.length;++d){if(j.sIO(d)){j.OCCUR=k;
|
||||
j.hC();j.go(j.S[d].J);return;}}j.warn("Search forwards: text not found.",false,j.OCCUR);
|
||||
j.OCCUR=g;return;}else{if(a=="S"){for(var d=j.N.J+1;d<j.S.length;++d){if(j.sIO(d)){j.hC();
|
||||
j.go(j.S[d].J);return;}}j.warn("Search forwards: text not found.",false,j.OCCUR);
|
||||
return;}else{if(a=="r"){if(""==k){return false;}if(j.SHO){j.rSH();}var g=j.OCCUR;
|
||||
j.OCCUR=k;var e=0;if(k==j.OCCUR){e++;}j.mSR();for(var d=j.N.J-e;d>-1;--d){if(j.sIO(d)){j.hC();
|
||||
j.go(j.S[d].J);return;}}j.warn("Search backwards: text not found.",false,j.OCCUR);
|
||||
j.OCCUR=g;return;}else{if(a=="R"){for(var d=j.N.J-1;d>-1;--d){k=j.rT(j.S[d].H.innerHTML);
|
||||
if(j.sIO(d)){j.hC();j.go(j.S[d].J);return;}}j.warn("Search backwards: text not found.",false,j.OCCUR);
|
||||
return;}else{if(a=="o"){if(""==k){return false;}if(j.SHO){j.rSH();}var g=j.OCCUR;
|
||||
j.OCCUR=k;j.mSR();var b=new Array();for(var d=0;d<j.S.length;++d){if(j.sIO(d)){b.push(d);
|
||||
}}if(0==b.length){j.warn("Occur: text not found.",false,j.OCCUR);j.OCCUR=g;return;
|
||||
}j.hC();if(j.PLAIN_VIEW!=j.VIEW){j.pV();}j.R.DRT=true;j.tG();for(var d=0;d<j.S.length;
|
||||
++d){OrgNode.sE(j.S[d].D);OrgNode.hE(j.S[d].F);}for(var d=(b.length-1);d>=1;--d){OrgNode.sE(j.S[b[d]].F);
|
||||
}j.ss(b[0]);}else{if(a==j.RC_O){var h=k.charAt(0);if("s"==h){j.sR(j.RC_NULL,"Org-link to this section:","[["+j.BU+j.dT()+"]["+document.title+", Sec. '"+j.rT(j.N.H.innerHTML)+"']]","C-c to copy, ");
|
||||
window.setTimeout(function(){org_html_manager.CI.select();},100);}else{if("o"==h){j.sR(j.RC_NULL,"Org-link, occurences of <i>""+j.OCCUR+""</i>:","[["+j.BU+"?OCCUR="+j.OCCUR+"]["+document.title+", occurences of '"+j.OCCUR+"']]","C-c to copy, ");
|
||||
window.setTimeout(function(){org_html_manager.CI.select();},100);}else{j.warn(h+": No such link type!");
|
||||
}}}else{if(a==j.RC_H){var h=k.charAt(0);if("s"==h){j.sR(j.RC_NULL,"HTML-link to this section:",'<a href="'+j.BU+j.dT()+'">'+document.title+", Sec. '"+j.rT(j.N.H.innerHTML)+"'</a>","C-c to copy, ");
|
||||
window.setTimeout(function(){org_html_manager.CI.select();},100);}else{if("o"==h){j.sR(j.RC_NULL,"HTML-link, occurences of <i>""+j.OCCUR+""</i>:",'<a href="'+j.BU+"?OCCUR="+j.OCCUR+'">'+document.title+", occurences of '"+j.OCCUR+"'</a>","C-c to copy, ");
|
||||
window.setTimeout(function(){org_html_manager.CI.select();},100);}else{j.warn(h+": No such link type!");
|
||||
}}}else{if(a==j.RC_P){var h=k.charAt(0);if("s"==h){j.sR(j.RC_NULL,"Plain-link to this section:",j.BU+j.dT(),"C-c to copy, ");
|
||||
window.setTimeout(function(){org_html_manager.CI.select();},100);}else{if("o"==h){j.sR(j.RC_NULL,"Plain-link, occurences of <i>""+j.OCCUR+""</i>:",j.BU+"?OCCUR="+j.OCCUR,"C-c to copy, ");
|
||||
window.setTimeout(function(){org_html_manager.CI.select();},100);}else{j.warn(h+": No such link type!");
|
||||
}}}}}}}}}}}},dT:function(b){if(null==b){b=this.N;}var c="#"+this.N.I;for(var a in b.iTF){if(!a.match(this.SIDX)){c=a;
|
||||
break;}}return c;},mSR:function(){var a=this.OCCUR.replace(/>/g,">").replace(/</g,"<").replace(/=/g,"\\=").replace(/\\/g,"\\\\").replace(/\?/g,"\\?").replace(/\)/g,"\\)").replace(/\(/g,"\\(").replace(/\./g,"[^<>]").replace(/\"/g,""");
|
||||
this.SCX=new RegExp(">([^<]*)?("+a+")([^>]*)?<","ig");},sIO:function(c){var b=this;
|
||||
var a=false;if(null!=b.S[c]){if(b.SCX.test(b.S[c].H.innerHTML)){a=true;b.sSH(b.S[c].H);
|
||||
b.S[c].HH=true;b.SHO=true;}if(b.SCX.test(b.S[c].F.innerHTML)){a=true;b.sSH(b.S[c].F);
|
||||
b.S[c].HH=true;b.SHO=true;}return a;}return false;},sSH:function(b){var a=b.innerHTML;
|
||||
b.innerHTML=a.replace(this.SCX,'>$1<span class="org-info-js_search-highlight">$2</span>$3<');
|
||||
},rSH:function(){var c=this;for(var b=0;b<c.S.length;++b){if(c.S[b].HH){while(c.SC_HLX.test(c.S[b].H.innerHTML)){var a=c.S[b].H.innerHTML;
|
||||
c.S[b].H.innerHTML=a.replace(c.SC_HLX,"$2");}while(c.SC_HLX.test(c.S[b].F.innerHTML)){var a=c.S[b].F.innerHTML;
|
||||
c.S[b].F.innerHTML=a.replace(c.SC_HLX,"$2");}c.S[b].HH=false;}}c.SHO=false;},hH:function(b){var a=parseInt(b);
|
||||
if(this.PLAIN_VIEW==this.VIEW&&this.MOUSE_HINT){if("underline"==this.MOUSE_HINT){this.S[a].H.style.borderBottom="1px dashed #666666";
|
||||
}else{this.S[a].H.style.backgroundColor=this.MOUSE_HINT;}}},unhH:function(b){var a=parseInt(b);
|
||||
if("underline"==this.MOUSE_HINT){this.S[a].H.style.borderBottom="";}else{this.S[a].H.style.backgroundColor="";
|
||||
}},showHelp:function(){var a=this;if(a.Rg){a.eR();}else{if(a.Mg){a.rW();}}a.Hg=a.Hg?0:1;
|
||||
if(a.Hg){a.LVM=a.VIEW;if(a.PLAIN_VIEW==a.VIEW){a.iV(true);}a.W.innerHTML='Press any key or <a href="javascript:org_html_manager.showHelp();">click here</a> to proceed.<h2>Keyboard Shortcuts</h2><table cellpadding="3" rules="groups" frame="hsides" style="caption-side:bottom;margin:20px;border-style:none;" border="0";><caption><small>org-info.js, v. 0.1.7.1</small></caption><tbody><tr><td><code><b>? / ¿</b></code></td><td>show this help screen</td></tr></tbody><tbody><tr><td><code><b></b></code></td><td><b>Moving around</b></td></tr><tr><td><code><b>n / p</b></code></td><td>goto the next / previous section</td></tr><tr><td><code><b>N / P</b></code></td><td>goto the next / previous sibling</td></tr><tr><td><code><b>t / E</b></code></td><td>goto the first / last section</td></tr><tr><td><code><b>g</b></code></td><td>goto section...</td></tr><tr><td><code><b>u</b></code></td><td>go one level up (parent section)</td></tr><tr><td><code><b>i / C</b></code></td><td>show table of contents / tags index</td></tr><tr><td><code><b>b / B</b></code></td><td>go back to last / forward to next visited section.</td></tr><tr><td><code><b>h / H</b></code></td><td>go to main index in this directory / link HOME page</td></tr></tbody><tbody><tr><td><code><b></b></code></td><td><b>View</b></td></tr><tr><td><code><b>m / x</b></code></td><td>toggle the view mode between info and plain / slides</td></tr><tr><td><code><b>f / F</b></code></td><td>fold current section / whole document (plain view only)</td></tr></tbody><tbody><tr><td><code><b></b></code></td><td><b>Searching</b></td></tr><tr><td><code><b>s / r</b></code></td><td>search forward / backward....</td></tr><tr><td><code><b>S / R</b></code></td><td>search again forward / backward</td></tr><tr><td><code><b>o</b></code></td><td>occur-mode</td></tr><tr><td><code><b>c</b></code></td><td>clear search-highlight</td></tr></tbody><tbody><tr><td><code><b></b></code></td><td><b>Misc</b></td></tr><tr><td><code><b>l / L / U</b></code></td><td>display HTML link / Org link / Plain-URL</td></tr><tr><td><code><b>v / V</b></code></td><td>scroll down / up</td></tr><tr><td><code><b>W</b></code></td><td>Print</td></tr></tbody></table><br />Press any key or <a href="javascript:org_html_manager.showHelp();">click here</a> to proceed.';
|
||||
window.scrollTo(0,0);}else{if(a.PLAIN_VIEW==a.LVM){a.pV();}else{if(a.SLIDE_VIEW==a.LVM){a.sV();
|
||||
}}a.ss(a.N.J);}},showTagsIndex:function(){var e=this;if(e.Rg){e.eR();}else{if(e.Mg){e.rW();
|
||||
}}e.Hg=e.Hg?0:1;if(e.Hg){e.LVM=e.VIEW;if(e.PLAIN_VIEW==e.VIEW){e.iV(true);}if(null==e.TAGS_INDEX){e.TAGS_INDEX='Press any key or <a href="javascript:org_html_manager.showTagsIndex();">click here</a> to proceed.<br /><br />Click the headlines to expand the contents.<h2>Index of Tags</h2>';
|
||||
for(var d=0;d<e.ST.length;++d){var b=e.ST[d];var f="org-html-manager-sorted-tags-"+b;
|
||||
e.TAGS_INDEX+="<a href=\"javascript:OrgNode.toggleElement(document.getElementById('"+f+"'));\"><h3>"+b+'</h3></a><div id="'+f+'" style="visibility:hidden;display:none;"><ul>';
|
||||
for(var c=0;c<e.TAGS[b].length;++c){var a=e.TAGS[b][c];e.TAGS_INDEX+='<li><a href="javascript:org_html_manager.ss('+a+');">'+e.S[a].H.innerHTML+"</a></li>";
|
||||
}e.TAGS_INDEX+="</ul></div>";}e.TAGS_INDEX+='<br />Press any key or <a href="javascript:org_html_manager.showTagsIndex();">click here</a> to proceed.';
|
||||
}e.W.innerHTML=e.TAGS_INDEX;window.scrollTo(0,0);}else{if(e.PLAIN_VIEW==e.LVM){e.pV();
|
||||
}else{if(e.SLIDE_VIEW==e.LVM){e.sV();}}e.ss(e.N.J);}},runHooks:function(b,a){if(this.HOOKS.run_hooks&&this.HOOKS[b]){for(var c=0;
|
||||
c<this.HOOKS[b].length;++c){this.HOOKS[b][c](this,a);}}},addHook:function(a,b){if("run_hooks"!=a){this.HOOKS[a].push(b);
|
||||
}},removeHook:function(a,c){if(this.HOOKS[a]){for(var b=this.HOOKS[a].length-1;b>=0;
|
||||
--b){if(this.HOOKS[a][b]==c){this.HOOKS[a].splice(b,1);}}}}};function OrgHtmlManagerKeyEvent(b){var d;
|
||||
if(!b){b=window.event;}if(b.which){d=b.which;}else{if(b.keyCode){d=b.keyCode;}}if(b.ctrlKey){return;
|
||||
}var a=String.fromCharCode(d);if(b.shiftKey){org_html_manager.CI.value=org_html_manager.CI.value+a;
|
||||
}else{org_html_manager.CI.value=org_html_manager.CI.value+a.toLowerCase();}org_html_manager.getKey();
|
||||
}function OrgHtmlManagerLoadCheck(){org_html_manager.init();}
|
||||
Loading…
Reference in New Issue
Block a user