linear_solver_oct_m Module Reference

Data Types
type	linear_solver_args_t
type	linear_solver_t

Functions/Subroutines
subroutine, public	linear_solver_init (this, namespace, gr, states_are_real, mc, space)
subroutine, public	linear_solver_end (this)
integer function, public	linear_solver_ops_per_iter (this)
subroutine, public	linear_solver_obsolete_variables (namespace, old_prefix, new_prefix)
subroutine, public	dlinear_solver_solve_hxey (this, namespace, hm, mesh, st, ist, ik, x, y, shift, tol, residue, iter_used, occ_response)
	This subroutine calculates the solution of (H + shift) x = y Typically shift = - eigenvalue + omega. More...
subroutine, public	dlinear_solver_solve_hxey_batch (this, namespace, hm, mesh, st, xb, yb, shift, tol, residue, iter_used, occ_response, use_initial_guess)
subroutine	dlinear_solver_cg (ls, namespace, hm, mesh, st, ist, ik, x, y, shift, tol, residue, iter_used)
	Conjugate gradients. More...
subroutine	dlinear_solver_idrs (ls, namespace, mesh, st, x, y, tol, residue, iter_used)
	IDRS This is the "Induced Dimension Reduction", IDR(s) (for s=4). IDR(s) is a robust and efficient short recurrence Krylov subspace method for solving large nonsymmetric systems of linear equations. It is described in [Peter Sonneveld and Martin B. van Gijzen, SIAM J. Sci. Comput. 31, 1035 (2008)]. We have adapted the code released by M. B. van Gizjen [http: More...
subroutine	dlinear_solver_bicgstab (ls, namespace, hm, mesh, st, ist, ik, x, y, shift, tol, residue, iter_used, occ_response)
	BICONJUGATE GRADIENTS STABILIZED see http: More...
subroutine	dlinear_solver_multigrid (ls, namespace, hm, mesh, st, ist, ik, x, y, shift, tol, residue, iter_used)
subroutine	dlinear_solver_operator (hm, namespace, mesh, st, ist, ik, shift, x, hx)
	This routine applies the operator hx = [H (+ Q) + shift] x. More...
subroutine	dlinear_solver_operator_batch (hm, namespace, mesh, st, shift, xb, hxb)
subroutine	dlinear_solver_operator_na (x, hx)
	applies linear_solver_operator with other arguments implicit as global variables More...
subroutine	dlinear_solver_operator_t_na (x, hx)
	applies transpose of linear_solver_operator with other arguments implicit as global variables \( (H - shift)^T = H* - shift = (H - shift*)* \) More...
subroutine	dlinear_solver_operator_sym_na (x, hx)
	applies linear_solver_operator in symmetrized form: \( A^T A \) More...
subroutine	dlinear_solver_preconditioner (x, hx)
subroutine	dlinear_solver_sos (hm, namespace, mesh, st, ist, ik, x, y, shift, residue, iter_used)
subroutine	dlinear_solver_qmr_dotp (this, namespace, hm, mesh, st, xb, bb, shift, iter_used, residue, threshold, use_initial_guess)
	for complex symmetric matrices W Chen and B Poirier, J Comput Phys 219, 198-209 (2006) More...
real(real64) function, dimension(n)	dsingledimarray (n, a)
real(real64) function, dimension(np, dim)	ddoubledimarray (np, dim, a)
real(real64) function	ddotproduct (a, b)
real(real64) function, dimension(size(v, 1), size(v, 2))	dmatrixvector (v)
real(real64) function, dimension(size(v, 1), size(v, 2))	dpreconditioner (v)
subroutine, public	zlinear_solver_solve_hxey (this, namespace, hm, mesh, st, ist, ik, x, y, shift, tol, residue, iter_used, occ_response)
	This subroutine calculates the solution of (H + shift) x = y Typically shift = - eigenvalue + omega. More...
subroutine, public	zlinear_solver_solve_hxey_batch (this, namespace, hm, mesh, st, xb, yb, shift, tol, residue, iter_used, occ_response, use_initial_guess)
subroutine	zlinear_solver_cg (ls, namespace, hm, mesh, st, ist, ik, x, y, shift, tol, residue, iter_used)
	Conjugate gradients. More...
subroutine	zlinear_solver_idrs (ls, namespace, mesh, st, x, y, tol, residue, iter_used)
	IDRS This is the "Induced Dimension Reduction", IDR(s) (for s=4). IDR(s) is a robust and efficient short recurrence Krylov subspace method for solving large nonsymmetric systems of linear equations. It is described in [Peter Sonneveld and Martin B. van Gijzen, SIAM J. Sci. Comput. 31, 1035 (2008)]. We have adapted the code released by M. B. van Gizjen [http: More...
subroutine	zlinear_solver_bicgstab (ls, namespace, hm, mesh, st, ist, ik, x, y, shift, tol, residue, iter_used, occ_response)
	BICONJUGATE GRADIENTS STABILIZED see http: More...
subroutine	zlinear_solver_multigrid (ls, namespace, hm, mesh, st, ist, ik, x, y, shift, tol, residue, iter_used)
subroutine	zlinear_solver_operator (hm, namespace, mesh, st, ist, ik, shift, x, hx)
	This routine applies the operator hx = [H (+ Q) + shift] x. More...
subroutine	zlinear_solver_operator_batch (hm, namespace, mesh, st, shift, xb, hxb)
subroutine	zlinear_solver_operator_na (x, hx)
	applies linear_solver_operator with other arguments implicit as global variables More...
subroutine	zlinear_solver_operator_t_na (x, hx)
	applies transpose of linear_solver_operator with other arguments implicit as global variables \( (H - shift)^T = H* - shift = (H - shift*)* \) More...
subroutine	zlinear_solver_operator_sym_na (x, hx)
	applies linear_solver_operator in symmetrized form: \( A^T A \) More...
subroutine	zlinear_solver_preconditioner (x, hx)
subroutine	zlinear_solver_sos (hm, namespace, mesh, st, ist, ik, x, y, shift, residue, iter_used)
subroutine	zlinear_solver_qmr_dotp (this, namespace, hm, mesh, st, xb, bb, shift, iter_used, residue, threshold, use_initial_guess)
	for complex symmetric matrices W Chen and B Poirier, J Comput Phys 219, 198-209 (2006) More...
complex(real64) function, dimension(n)	zsingledimarray (n, a)
complex(real64) function, dimension(np, dim)	zdoubledimarray (np, dim, a)
complex(real64) function	zdotproduct (a, b)
complex(real64) function, dimension(size(v, 1), size(v, 2))	zmatrixvector (v)
complex(real64) function, dimension(size(v, 1), size(v, 2))	zpreconditioner (v)

Variables
type(linear_solver_args_t)	args

Function/Subroutine Documentation

linear_solver_init()

subroutine, public linear_solver_oct_m::linear_solver_init	(	type(linear_solver_t), intent(out)	this,
		type(namespace_t), intent(in)	namespace,
		type(grid_t), intent(inout)	gr,
		logical, intent(in)	states_are_real,
		type(multicomm_t), intent(in)	mc,
		class(space_t), intent(in)	space
	)

Parameters

[in]

states_are_real

for choosing solver

Definition at line 183 of file linear_solver.F90.

linear_solver_end()

subroutine, public linear_solver_oct_m::linear_solver_end

(

type(linear_solver_t), intent(inout)

this

)

Definition at line 321 of file linear_solver.F90.

linear_solver_ops_per_iter()

integer function, public linear_solver_oct_m::linear_solver_ops_per_iter

(

type(linear_solver_t), intent(inout)

this

)

Definition at line 335 of file linear_solver.F90.

linear_solver_obsolete_variables()

subroutine, public linear_solver_oct_m::linear_solver_obsolete_variables	(	type(namespace_t), intent(in)	namespace,
		character(len=*), intent(in)	old_prefix,
		character(len=*), intent(in)	new_prefix
	)

Definition at line 349 of file linear_solver.F90.

dlinear_solver_solve_hxey()

subroutine, public linear_solver_oct_m::dlinear_solver_solve_hxey	(	type(linear_solver_t), intent(inout), target	this,
		type(namespace_t), intent(in), target	namespace,
		type(hamiltonian_elec_t), intent(in), target	hm,
		class(mesh_t), intent(in), target	mesh,
		type(states_elec_t), intent(in), target	st,
		integer, intent(in)	ist,
		integer, intent(in)	ik,
		real(real64), dimension(:,:), intent(inout), contiguous	x,
		real(real64), dimension(:,:), intent(in), contiguous	y,
		real(real64), intent(in)	shift,
		real(real64), intent(in)	tol,
		real(real64), intent(out)	residue,
		integer, intent(out)	iter_used,
		logical, intent(in), optional	occ_response
	)

This subroutine calculates the solution of (H + shift) x = y Typically shift = - eigenvalue + omega.

Parameters

[in,out]	x	x(meshnp_part, ddim)
[in]	y	y(meshnp, ddim)

Definition at line 434 of file linear_solver.F90.

dlinear_solver_solve_hxey_batch()

subroutine, public linear_solver_oct_m::dlinear_solver_solve_hxey_batch	(	type(linear_solver_t), intent(inout), target	this,
		type(namespace_t), intent(in)	namespace,
		type(hamiltonian_elec_t), intent(in), target	hm,
		class(mesh_t), intent(in), target	mesh,
		type(states_elec_t), intent(in), target	st,
		type(wfs_elec_t), intent(inout)	xb,
		type(wfs_elec_t), intent(inout)	yb,
		real(real64), dimension(:), intent(in), contiguous	shift,
		real(real64), intent(in)	tol,
		real(real64), dimension(:), intent(out), contiguous	residue,
		integer, dimension(:), intent(out)	iter_used,
		logical, intent(in), optional	occ_response,
		logical, intent(in), optional	use_initial_guess
	)

Definition at line 525 of file linear_solver.F90.

dlinear_solver_cg()

subroutine linear_solver_oct_m::dlinear_solver_cg ( type(linear_solver_t), intent(inout)  ls, type(namespace_t), intent(in)  namespace, type(hamiltonian_elec_t), intent(in)  hm, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, integer, intent(in)  ist, integer, intent(in)  ik, real(real64), dimension(:,:), intent(inout), contiguous  x, real(real64), dimension(:,:), intent(in), contiguous  y, real(real64), intent(in)  shift, real(real64), intent(in)  tol, real(real64), intent(out)  residue, integer, intent(out)  iter_used  )

private

Conjugate gradients.

Parameters

[in,out]	x	x(meshnp, stddim)
[in]	y	y(meshnp, stddim)

Definition at line 576 of file linear_solver.F90.

dlinear_solver_idrs()

subroutine linear_solver_oct_m::dlinear_solver_idrs ( type(linear_solver_t), intent(inout)  ls, type(namespace_t), intent(in)  namespace, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, real(real64), dimension(:,:), intent(inout), contiguous  x, real(real64), dimension(:,:), intent(in), contiguous  y, real(real64), intent(in)  tol, real(real64), intent(out)  residue, integer, intent(out)  iter_used  )

private

IDRS This is the "Induced Dimension Reduction", IDR(s) (for s=4). IDR(s) is a robust and efficient short recurrence Krylov subspace method for solving large nonsymmetric systems of linear equations. It is described in [Peter Sonneveld and Martin B. van Gijzen, SIAM J. Sci. Comput. 31, 1035 (2008)]. We have adapted the code released by M. B. van Gizjen [http:

Parameters

[in,out]	x	x(meshnp, stddim)
[in]	y	y(meshnp, stddim)

Definition at line 666 of file linear_solver.F90.

dlinear_solver_bicgstab()

subroutine linear_solver_oct_m::dlinear_solver_bicgstab ( type(linear_solver_t), intent(inout)  ls, type(namespace_t), intent(in)  namespace, type(hamiltonian_elec_t), intent(in)  hm, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, integer, intent(in)  ist, integer, intent(in)  ik, real(real64), dimension(:,:), intent(inout), contiguous  x, real(real64), dimension(:,:), intent(in), contiguous  y, real(real64), intent(in)  shift, real(real64), intent(in)  tol, real(real64), intent(out)  residue, integer, intent(out)  iter_used, logical, intent(in)  occ_response  )

private

BICONJUGATE GRADIENTS STABILIZED see http:

Parameters

[in,out]	x	x(meshnp, stddim)
[in]	y	y(meshnp, stddim)

Definition at line 712 of file linear_solver.F90.

dlinear_solver_multigrid()

subroutine linear_solver_oct_m::dlinear_solver_multigrid ( type(linear_solver_t), intent(inout)  ls, type(namespace_t), intent(in)  namespace, type(hamiltonian_elec_t), intent(in)  hm, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, integer, intent(in)  ist, integer, intent(in)  ik, real(real64), dimension(:,:), intent(inout), contiguous  x, real(real64), dimension(:,:), intent(in), contiguous  y, real(real64), intent(in)  shift, real(real64), intent(in)  tol, real(real64), intent(out)  residue, integer, intent(out)  iter_used  )

private

Definition at line 864 of file linear_solver.F90.

dlinear_solver_operator()

subroutine linear_solver_oct_m::dlinear_solver_operator ( type(hamiltonian_elec_t), intent(in)  hm, type(namespace_t), intent(in)  namespace, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, integer, intent(in)  ist, integer, intent(in)  ik, real(real64), intent(in)  shift, real(real64), dimension(:,:), intent(inout), contiguous  x, real(real64), dimension(:,:), intent(out), contiguous  hx  )

private

This routine applies the operator hx = [H (+ Q) + shift] x.

Parameters

[in,out]	x	x(meshnp_part, stddim)
[out]	hx	Hx(meshnp, stddim)

Definition at line 960 of file linear_solver.F90.

dlinear_solver_operator_batch()

subroutine linear_solver_oct_m::dlinear_solver_operator_batch ( type(hamiltonian_elec_t), intent(in)  hm, type(namespace_t), intent(in)  namespace, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, real(real64), dimension(:), intent(in)  shift, type(wfs_elec_t), intent(inout)  xb, type(wfs_elec_t), intent(inout)  hxb  )

private

Definition at line 1010 of file linear_solver.F90.

dlinear_solver_operator_na()

subroutine linear_solver_oct_m::dlinear_solver_operator_na ( real(real64), dimension(:), intent(in), contiguous  x, real(real64), dimension(:), intent(out), contiguous  hx  )

private

applies linear_solver_operator with other arguments implicit as global variables

Parameters

[in]	x	x(meshnp, stddim)
[out]	hx	Hx(meshnp, stddim)

Definition at line 1068 of file linear_solver.F90.

dlinear_solver_operator_t_na()

subroutine linear_solver_oct_m::dlinear_solver_operator_t_na ( real(real64), dimension(:), intent(in), contiguous  x, real(real64), dimension(:), intent(out), contiguous  hx  )

private

applies transpose of linear_solver_operator with other arguments implicit as global variables \( (H - shift)^T = H* - shift = (H - shift*)* \)

Definition at line 1091 of file linear_solver.F90.

dlinear_solver_operator_sym_na()

subroutine linear_solver_oct_m::dlinear_solver_operator_sym_na ( real(real64), dimension(:), intent(in), contiguous  x, real(real64), dimension(:), intent(out), contiguous  hx  )

private

applies linear_solver_operator in symmetrized form: \( A^T A \)

Parameters

[in]	x	x(meshnp, stddim)
[out]	hx	Hx(meshnp, stddim)

Definition at line 1113 of file linear_solver.F90.

dlinear_solver_preconditioner()

subroutine linear_solver_oct_m::dlinear_solver_preconditioner ( real(real64), dimension(:), intent(in), contiguous  x, real(real64), dimension(:), intent(out), contiguous  hx  )

private

Parameters

[in]	x	x(meshnp, stddim)
[out]	hx	Hx(meshnp, stddim)

Definition at line 1137 of file linear_solver.F90.

dlinear_solver_sos()

subroutine linear_solver_oct_m::dlinear_solver_sos ( type(hamiltonian_elec_t), intent(in)  hm, type(namespace_t), intent(in)  namespace, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, integer, intent(in)  ist, integer, intent(in)  ik, real(real64), dimension(:,:), intent(inout), contiguous  x, real(real64), dimension(:,:), intent(in), contiguous  y, real(real64), intent(in)  shift, real(real64), intent(out)  residue, integer, intent(out)  iter_used  )

private

Parameters

[in,out]	x	x(meshnp, stddim)
[in]	y	y(meshnp, stddim)

Definition at line 1160 of file linear_solver.F90.

dlinear_solver_qmr_dotp()

subroutine linear_solver_oct_m::dlinear_solver_qmr_dotp ( type(linear_solver_t), intent(inout)  this, type(namespace_t), intent(in)  namespace, type(hamiltonian_elec_t), intent(in)  hm, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, type(wfs_elec_t), intent(inout)  xb, type(wfs_elec_t), intent(in)  bb, real(real64), dimension(:), intent(in)  shift, integer, dimension(:), intent(out)  iter_used, real(real64), dimension(:), intent(out), contiguous  residue, real(real64), intent(in)  threshold, logical, intent(in), optional  use_initial_guess  )

private

for complex symmetric matrices W Chen and B Poirier, J Comput Phys 219, 198-209 (2006)

Parameters

[out]	residue	the residue = abs(Ax-b)
[in]	threshold	convergence threshold

Definition at line 1217 of file linear_solver.F90.

dsingledimarray()

real(real64) function, dimension(n) linear_solver_oct_m::dsingledimarray ( integer, intent(in)  n, real(real64), dimension(:, :), intent(in)  a  )

private

Definition at line 1584 of file linear_solver.F90.

ddoubledimarray()

real(real64) function, dimension(np, dim) linear_solver_oct_m::ddoubledimarray ( integer, intent(in)  np, integer, intent(in)  dim, real(real64), dimension(:), intent(in)  a  )

private

Definition at line 1596 of file linear_solver.F90.

ddotproduct()

real(real64) function linear_solver_oct_m::ddotproduct ( real(real64), dimension(:), intent(in)  a, real(real64), dimension(:), intent(in)  b  )

private

Definition at line 1606 of file linear_solver.F90.

dmatrixvector()

real(real64) function, dimension(size(v, 1), size(v, 2)) linear_solver_oct_m::dmatrixvector ( real(real64), dimension(:, :), intent(in)  v )

private

Definition at line 1613 of file linear_solver.F90.

dpreconditioner()

real(real64) function, dimension(size(v, 1), size(v, 2)) linear_solver_oct_m::dpreconditioner ( real(real64), dimension(:, :), intent(in)  v )

private

Definition at line 1636 of file linear_solver.F90.

zlinear_solver_solve_hxey()

subroutine, public linear_solver_oct_m::zlinear_solver_solve_hxey	(	type(linear_solver_t), intent(inout), target	this,
		type(namespace_t), intent(in), target	namespace,
		type(hamiltonian_elec_t), intent(in), target	hm,
		class(mesh_t), intent(in), target	mesh,
		type(states_elec_t), intent(in), target	st,
		integer, intent(in)	ist,
		integer, intent(in)	ik,
		complex(real64), dimension(:,:), intent(inout), contiguous	x,
		complex(real64), dimension(:,:), intent(in), contiguous	y,
		complex(real64), intent(in)	shift,
		real(real64), intent(in)	tol,
		real(real64), intent(out)	residue,
		integer, intent(out)	iter_used,
		logical, intent(in), optional	occ_response
	)

This subroutine calculates the solution of (H + shift) x = y Typically shift = - eigenvalue + omega.

Parameters

[in,out]	x	x(meshnp_part, ddim)
[in]	y	y(meshnp, ddim)

Definition at line 1738 of file linear_solver.F90.

zlinear_solver_solve_hxey_batch()

subroutine, public linear_solver_oct_m::zlinear_solver_solve_hxey_batch	(	type(linear_solver_t), intent(inout), target	this,
		type(namespace_t), intent(in)	namespace,
		type(hamiltonian_elec_t), intent(in), target	hm,
		class(mesh_t), intent(in), target	mesh,
		type(states_elec_t), intent(in), target	st,
		type(wfs_elec_t), intent(inout)	xb,
		type(wfs_elec_t), intent(inout)	yb,
		complex(real64), dimension(:), intent(in), contiguous	shift,
		real(real64), intent(in)	tol,
		real(real64), dimension(:), intent(out), contiguous	residue,
		integer, dimension(:), intent(out)	iter_used,
		logical, intent(in), optional	occ_response,
		logical, intent(in), optional	use_initial_guess
	)

Definition at line 1829 of file linear_solver.F90.

zlinear_solver_cg()

subroutine linear_solver_oct_m::zlinear_solver_cg ( type(linear_solver_t), intent(inout)  ls, type(namespace_t), intent(in)  namespace, type(hamiltonian_elec_t), intent(in)  hm, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, integer, intent(in)  ist, integer, intent(in)  ik, complex(real64), dimension(:,:), intent(inout), contiguous  x, complex(real64), dimension(:,:), intent(in), contiguous  y, complex(real64), intent(in)  shift, real(real64), intent(in)  tol, real(real64), intent(out)  residue, integer, intent(out)  iter_used  )

private

Conjugate gradients.

Parameters

[in,out]	x	x(meshnp, stddim)
[in]	y	y(meshnp, stddim)

Definition at line 1880 of file linear_solver.F90.

zlinear_solver_idrs()

subroutine linear_solver_oct_m::zlinear_solver_idrs ( type(linear_solver_t), intent(inout)  ls, type(namespace_t), intent(in)  namespace, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, complex(real64), dimension(:,:), intent(inout), contiguous  x, complex(real64), dimension(:,:), intent(in), contiguous  y, real(real64), intent(in)  tol, real(real64), intent(out)  residue, integer, intent(out)  iter_used  )

private

IDRS This is the "Induced Dimension Reduction", IDR(s) (for s=4). IDR(s) is a robust and efficient short recurrence Krylov subspace method for solving large nonsymmetric systems of linear equations. It is described in [Peter Sonneveld and Martin B. van Gijzen, SIAM J. Sci. Comput. 31, 1035 (2008)]. We have adapted the code released by M. B. van Gizjen [http:

Parameters

[in,out]	x	x(meshnp, stddim)
[in]	y	y(meshnp, stddim)

Definition at line 1970 of file linear_solver.F90.

zlinear_solver_bicgstab()

subroutine linear_solver_oct_m::zlinear_solver_bicgstab ( type(linear_solver_t), intent(inout)  ls, type(namespace_t), intent(in)  namespace, type(hamiltonian_elec_t), intent(in)  hm, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, integer, intent(in)  ist, integer, intent(in)  ik, complex(real64), dimension(:,:), intent(inout), contiguous  x, complex(real64), dimension(:,:), intent(in), contiguous  y, complex(real64), intent(in)  shift, real(real64), intent(in)  tol, real(real64), intent(out)  residue, integer, intent(out)  iter_used, logical, intent(in)  occ_response  )

private

BICONJUGATE GRADIENTS STABILIZED see http:

Parameters

[in,out]	x	x(meshnp, stddim)
[in]	y	y(meshnp, stddim)

Definition at line 2016 of file linear_solver.F90.

zlinear_solver_multigrid()

subroutine linear_solver_oct_m::zlinear_solver_multigrid ( type(linear_solver_t), intent(inout)  ls, type(namespace_t), intent(in)  namespace, type(hamiltonian_elec_t), intent(in)  hm, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, integer, intent(in)  ist, integer, intent(in)  ik, complex(real64), dimension(:,:), intent(inout), contiguous  x, complex(real64), dimension(:,:), intent(in), contiguous  y, complex(real64), intent(in)  shift, real(real64), intent(in)  tol, real(real64), intent(out)  residue, integer, intent(out)  iter_used  )

private

Definition at line 2168 of file linear_solver.F90.

zlinear_solver_operator()

subroutine linear_solver_oct_m::zlinear_solver_operator ( type(hamiltonian_elec_t), intent(in)  hm, type(namespace_t), intent(in)  namespace, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, integer, intent(in)  ist, integer, intent(in)  ik, complex(real64), intent(in)  shift, complex(real64), dimension(:,:), intent(inout), contiguous  x, complex(real64), dimension(:,:), intent(out), contiguous  hx  )

private

This routine applies the operator hx = [H (+ Q) + shift] x.

Parameters

[in,out]	x	x(meshnp_part, stddim)
[out]	hx	Hx(meshnp, stddim)

Definition at line 2264 of file linear_solver.F90.

zlinear_solver_operator_batch()

subroutine linear_solver_oct_m::zlinear_solver_operator_batch ( type(hamiltonian_elec_t), intent(in)  hm, type(namespace_t), intent(in)  namespace, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, complex(real64), dimension(:), intent(in)  shift, type(wfs_elec_t), intent(inout)  xb, type(wfs_elec_t), intent(inout)  hxb  )

private

Definition at line 2314 of file linear_solver.F90.

zlinear_solver_operator_na()

subroutine linear_solver_oct_m::zlinear_solver_operator_na ( complex(real64), dimension(:), intent(in), contiguous  x, complex(real64), dimension(:), intent(out), contiguous  hx  )

private

applies linear_solver_operator with other arguments implicit as global variables

Parameters

[in]	x	x(meshnp, stddim)
[out]	hx	Hx(meshnp, stddim)

Definition at line 2372 of file linear_solver.F90.

zlinear_solver_operator_t_na()

subroutine linear_solver_oct_m::zlinear_solver_operator_t_na ( complex(real64), dimension(:), intent(in), contiguous  x, complex(real64), dimension(:), intent(out), contiguous  hx  )

private

applies transpose of linear_solver_operator with other arguments implicit as global variables \( (H - shift)^T = H* - shift = (H - shift*)* \)

Definition at line 2395 of file linear_solver.F90.

zlinear_solver_operator_sym_na()

subroutine linear_solver_oct_m::zlinear_solver_operator_sym_na ( complex(real64), dimension(:), intent(in), contiguous  x, complex(real64), dimension(:), intent(out), contiguous  hx  )

private

applies linear_solver_operator in symmetrized form: \( A^T A \)

Parameters

[in]	x	x(meshnp, stddim)
[out]	hx	Hx(meshnp, stddim)

Definition at line 2417 of file linear_solver.F90.

zlinear_solver_preconditioner()

subroutine linear_solver_oct_m::zlinear_solver_preconditioner ( complex(real64), dimension(:), intent(in), contiguous  x, complex(real64), dimension(:), intent(out), contiguous  hx  )

private

Parameters

[in]	x	x(meshnp, stddim)
[out]	hx	Hx(meshnp, stddim)

Definition at line 2441 of file linear_solver.F90.

zlinear_solver_sos()

subroutine linear_solver_oct_m::zlinear_solver_sos ( type(hamiltonian_elec_t), intent(in)  hm, type(namespace_t), intent(in)  namespace, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, integer, intent(in)  ist, integer, intent(in)  ik, complex(real64), dimension(:,:), intent(inout), contiguous  x, complex(real64), dimension(:,:), intent(in), contiguous  y, complex(real64), intent(in)  shift, real(real64), intent(out)  residue, integer, intent(out)  iter_used  )

private

Parameters

[in,out]	x	x(meshnp, stddim)
[in]	y	y(meshnp, stddim)

Definition at line 2464 of file linear_solver.F90.

zlinear_solver_qmr_dotp()

subroutine linear_solver_oct_m::zlinear_solver_qmr_dotp ( type(linear_solver_t), intent(inout)  this, type(namespace_t), intent(in)  namespace, type(hamiltonian_elec_t), intent(in)  hm, class(mesh_t), intent(in)  mesh, type(states_elec_t), intent(in)  st, type(wfs_elec_t), intent(inout)  xb, type(wfs_elec_t), intent(in)  bb, complex(real64), dimension(:), intent(in)  shift, integer, dimension(:), intent(out)  iter_used, real(real64), dimension(:), intent(out), contiguous  residue, real(real64), intent(in)  threshold, logical, intent(in), optional  use_initial_guess  )

private

for complex symmetric matrices W Chen and B Poirier, J Comput Phys 219, 198-209 (2006)

Parameters

[out]	residue	the residue = abs(Ax-b)
[in]	threshold	convergence threshold

Definition at line 2521 of file linear_solver.F90.

zsingledimarray()

complex(real64) function, dimension(n) linear_solver_oct_m::zsingledimarray ( integer, intent(in)  n, complex(real64), dimension(:, :), intent(in)  a  )

private

Definition at line 2888 of file linear_solver.F90.

zdoubledimarray()

complex(real64) function, dimension(np, dim) linear_solver_oct_m::zdoubledimarray ( integer, intent(in)  np, integer, intent(in)  dim, complex(real64), dimension(:), intent(in)  a  )

private

Definition at line 2900 of file linear_solver.F90.

zdotproduct()

complex(real64) function linear_solver_oct_m::zdotproduct ( complex(real64), dimension(:), intent(in)  a, complex(real64), dimension(:), intent(in)  b  )

private

Definition at line 2910 of file linear_solver.F90.

zmatrixvector()

complex(real64) function, dimension(size(v, 1), size(v, 2)) linear_solver_oct_m::zmatrixvector ( complex(real64), dimension(:, :), intent(in)  v )

private

Definition at line 2917 of file linear_solver.F90.

zpreconditioner()

complex(real64) function, dimension(size(v, 1), size(v, 2)) linear_solver_oct_m::zpreconditioner ( complex(real64), dimension(:, :), intent(in)  v )

private

Definition at line 2940 of file linear_solver.F90.

Variable Documentation

args

type(linear_solver_args_t) linear_solver_oct_m::args

private

Definition at line 178 of file linear_solver.F90.