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authorDaniel Baumann <daniel.baumann@progress-linux.org>2024-03-09 13:19:48 +0000
committerDaniel Baumann <daniel.baumann@progress-linux.org>2024-03-09 13:20:02 +0000
commit58daab21cd043e1dc37024a7f99b396788372918 (patch)
tree96771e43bb69f7c1c2b0b4f7374cb74d7866d0cb /ml/dlib/dlib/quantum_computing/quantum_computing_abstract.h
parentReleasing debian version 1.43.2-1. (diff)
downloadnetdata-58daab21cd043e1dc37024a7f99b396788372918.tar.xz
netdata-58daab21cd043e1dc37024a7f99b396788372918.zip
Merging upstream version 1.44.3.
Signed-off-by: Daniel Baumann <daniel.baumann@progress-linux.org>
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+// Copyright (C) 2008 Davis E. King (davis@dlib.net)
+// License: Boost Software License See LICENSE.txt for the full license.
+#undef DLIB_QUANTUM_COMPUTINg_ABSTRACT_
+#ifdef DLIB_QUANTUM_COMPUTINg_ABSTRACT_
+
+#include <complex>
+#include "../matrix.h"
+#include "../rand.h"
+
+namespace dlib
+{
+
+// ----------------------------------------------------------------------------------------
+
+ typedef std::complex<double> qc_scalar_type;
+
+// ----------------------------------------------------------------------------------------
+
+ class quantum_register
+ {
+ /*!
+ INITIAL VALUE
+ - num_bits() == 1
+ - state_vector().nr() == 2
+ - state_vector().nc() == 1
+ - state_vector()(0) == 1
+ - state_vector()(1) == 0
+ - probability_of_bit(0) == 0
+
+ - i.e. This register represents a single quantum bit and it is
+ completely in the 0 state.
+
+ WHAT THIS OBJECT REPRESENTS
+ This object represents a set of quantum bits.
+ !*/
+
+ public:
+
+ quantum_register(
+ );
+ /*!
+ ensures
+ - this object is properly initialized
+ !*/
+
+ int num_bits (
+ ) const;
+ /*!
+ ensures
+ - returns the number of quantum bits in this register
+ !*/
+
+ void set_num_bits (
+ int new_num_bits
+ );
+ /*!
+ requires
+ - 1 <= new_num_bits <= 30
+ ensures
+ - #num_bits() == new_num_bits
+ - #state_vector().nr() == 2^new_num_bits
+ (i.e. the size of the state_vector is exponential in the number of bits in a register)
+ - for all valid i:
+ - probability_of_bit(i) == 0
+ !*/
+
+ void zero_all_bits(
+ );
+ /*!
+ ensures
+ - for all valid i:
+ - probability_of_bit(i) == 0
+ !*/
+
+ void append (
+ const quantum_register& reg
+ );
+ /*!
+ ensures
+ - #num_bits() == num_bits() + reg.num_bits()
+ - #this->state_vector() == tensor_product(this->state_vector(), reg.state_vector())
+ - The original bits in *this become the high order bits of the resulting
+ register and all the bits in reg end up as the low order bits in the
+ resulting register.
+ !*/
+
+ double probability_of_bit (
+ int bit
+ ) const;
+ /*!
+ requires
+ - 0 <= bit < num_bits()
+ ensures
+ - returns the probability of measuring the given bit and it being in the 1 state.
+ - The returned value is also equal to the sum of norm(state_vector()(i)) for all
+ i where the bit'th bit in i is set to 1. (note that the lowest order bit is bit 0)
+ !*/
+
+ template <typename rand_type>
+ bool measure_bit (
+ int bit,
+ rand_type& rnd
+ );
+ /*!
+ requires
+ - 0 <= bit < num_bits()
+ - rand_type == an implementation of dlib/rand/rand_float_abstract.h
+ ensures
+ - measures the given bit in this register. Let R denote the boolean
+ result of the measurement, where true means the bit was measured to
+ have value 1 and false means it had a value of 0.
+ - if (R == true) then
+ - returns true
+ - #probability_of_bit(bit) == 1
+ - else
+ - returns false
+ - #probability_of_bit(bit) == 0
+ !*/
+
+ template <typename rand_type>
+ bool measure_and_remove_bit (
+ int bit,
+ rand_type& rnd
+ );
+ /*!
+ requires
+ - num_bits() > 1
+ - 0 <= bit < num_bits()
+ - rand_type == an implementation of dlib/rand/rand_float_abstract.h
+ ensures
+ - measures the given bit in this register. Let R denote the boolean
+ result of the measurement, where true means the bit was measured to
+ have value 1 and false means it had a value of 0.
+ - #num_bits() == num_bits() - 1
+ - removes the bit that was measured from this register.
+ - if (R == true) then
+ - returns true
+ - else
+ - returns false
+ !*/
+
+ const matrix<qc_scalar_type,0,1>& state_vector(
+ ) const;
+ /*!
+ ensures
+ - returns a const reference to the state vector that describes the state of
+ the quantum bits in this register.
+ !*/
+
+ matrix<qc_scalar_type,0,1>& state_vector(
+ );
+ /*!
+ ensures
+ - returns a non-const reference to the state vector that describes the state of
+ the quantum bits in this register.
+ !*/
+
+ void swap (
+ quantum_register& item
+ );
+ /*!
+ ensures
+ - swaps *this and item
+ !*/
+
+ };
+
+ inline void swap (
+ quantum_register& a,
+ quantum_register& b
+ ) { a.swap(b); }
+ /*!
+ provides a global swap function
+ !*/
+
+// ----------------------------------------------------------------------------------------
+
+ template <typename T>
+ class gate_exp
+ {
+ /*!
+ REQUIREMENTS ON T
+ T must be some object that inherits from gate_exp and implements its own
+ version of operator() and compute_state_element().
+
+ WHAT THIS OBJECT REPRESENTS
+ This object represents an expression that evaluates to a quantum gate
+ that operates on T::num_bits qubits.
+
+ This object makes it easy to create new types of gate objects. All
+ you need to do is inherit from gate_exp in the proper way and
+ then you can use your new gate objects in conjunction with all the
+ others.
+ !*/
+
+ public:
+
+ static const long num_bits = T::num_bits;
+ static const long dims = T::dims;
+
+ gate_exp(
+ T& exp
+ );
+ /*!
+ ensures
+ - #&ref() == &exp
+ !*/
+
+ const qc_scalar_type operator() (
+ long r,
+ long c
+ ) const;
+ /*!
+ requires
+ - 0 <= r < dims
+ - 0 <= c < dims
+ ensures
+ - returns ref()(r,c)
+ !*/
+
+ void apply_gate_to (
+ quantum_register& reg
+ ) const;
+ /*!
+ requires
+ - reg.num_bits() == num_bits
+ ensures
+ - applies this quantum gate to the given quantum register
+ - Let M represent the matrix for this quantum gate, then
+ #reg().state_vector() = M*reg().state_vector()
+ !*/
+
+ template <typename exp>
+ qc_scalar_type compute_state_element (
+ const matrix_exp<exp>& reg,
+ long row_idx
+ ) const;
+ /*!
+ requires
+ - reg.nr() == dims
+ - reg.nc() == 1
+ - 0 <= row_idx < dims
+ ensures
+ - Let M represent the matrix for this gate, then
+ this function returns rowm(M*reg, row_idx)
+ (i.e. returns the row_idx row of what you get when you apply this
+ gate to the given column vector in reg)
+ - This function works by calling ref().compute_state_element(reg,row_idx)
+ !*/
+
+ const T& ref(
+ );
+ /*!
+ ensures
+ - returns a reference to the subexpression contained in this object
+ !*/
+
+ const matrix<qc_scalar_type> mat (
+ ) const;
+ /*!
+ ensures
+ - returns a dense matrix object that contains the matrix for this gate
+ !*/
+ };
+
+// ----------------------------------------------------------------------------------------
+
+ template <typename T, typename U>
+ class composite_gate : public gate_exp<composite_gate<T,U> >
+ {
+ /*!
+ REQUIREMENTS ON T AND U
+ Both must be gate expressions that inherit from gate_exp
+
+ WHAT THIS OBJECT REPRESENTS
+ This object represents a quantum gate that is the tensor product of
+ two other quantum gates.
+
+
+ As an example, suppose you have 3 registers, reg_high, reg_low, and reg_all. Also
+ suppose that reg_all is what you get when you append reg_high and reg_low,
+ so reg_all.state_vector() == tensor_product(reg_high.state_vector(),reg_low.state_vector()).
+
+ Then applying a composite gate to reg_all would give you the same thing as
+ applying the lhs gate to reg_high and the rhs gate to reg_low and then appending
+ the two resulting registers. So the lhs gate of a composite_gate applies to
+ the high order bits of a regitser and the rhs gate applies to the lower order bits.
+ !*/
+ public:
+
+ composite_gate (
+ const composite_gate& g
+ );
+ /*!
+ ensures
+ - *this is a copy of g
+ !*/
+
+ composite_gate(
+ const gate_exp<T>& lhs_,
+ const gate_exp<U>& rhs_
+ ):
+ /*!
+ ensures
+ - #lhs == lhs_.ref()
+ - #rhs == rhs_.ref()
+ - #num_bits == T::num_bits + U::num_bits
+ - #dims == 2^num_bits
+ - #&ref() == this
+ !*/
+
+ const qc_scalar_type operator() (
+ long r,
+ long c
+ ) const;
+ /*!
+ requires
+ - 0 <= r < dims
+ - 0 <= c < dims
+ ensures
+ - Let M denote the tensor product of lhs with rhs, then this function
+ returns M(r,c)
+ (i.e. returns lhs(r/U::dims,c/U::dims)*rhs(r%U::dims, c%U::dims))
+ !*/
+
+ template <typename exp>
+ qc_scalar_type compute_state_element (
+ const matrix_exp<exp>& reg,
+ long row_idx
+ ) const;
+ /*!
+ requires
+ - reg.nr() == dims
+ - reg.nc() == 1
+ - 0 <= row_idx < dims
+ ensures
+ - Let M represent the matrix for this gate, then this function
+ returns rowm(M*reg, row_idx)
+ (i.e. returns the row_idx row of what you get when you apply this
+ gate to the given column vector in reg)
+ - This function works by calling rhs.compute_state_element() and using elements
+ of the matrix in lhs.
+ !*/
+
+ static const long num_bits;
+ static const long dims;
+
+ const T lhs;
+ const U rhs;
+ };
+
+// ----------------------------------------------------------------------------------------
+
+ template <long bits>
+ class gate : public gate_exp<gate<bits> >
+ {
+ /*!
+ REQUIREMENTS ON bits
+ 0 < bits <= 30
+
+ WHAT THIS OBJECT REPRESENTS
+ This object represents a quantum gate that operates on bits qubits.
+ It stores its gate matrix explicitly in a dense in-memory matrix.
+ !*/
+
+ public:
+ gate(
+ );
+ /*!
+ ensures
+ - num_bits == bits
+ - dims == 2^bits
+ - #&ref() == this
+ - for all valid r and c:
+ #(*this)(r,c) == 0
+ !*/
+
+ gate (
+ const gate& g
+ );
+ /*!
+ ensures
+ - *this is a copy of g
+ !*/
+
+ template <typename T>
+ explicit gate(
+ const gate_exp<T>& g
+ );
+ /*!
+ requires
+ - T::num_bits == num_bits
+ ensures
+ - num_bits == bits
+ - dims == 2^bits
+ - #&ref() == this
+ - for all valid r and c:
+ #(*this)(r,c) == g(r,c)
+ !*/
+
+ const qc_scalar_type& operator() (
+ long r,
+ long c
+ ) const;
+ /*!
+ requires
+ - 0 <= r < dims
+ - 0 <= c < dims
+ ensures
+ - Let M denote the matrix for this gate, then this function
+ returns a const reference to M(r,c)
+ !*/
+
+ qc_scalar_type& operator() (
+ long r,
+ long c
+ );
+ /*!
+ requires
+ - 0 <= r < dims
+ - 0 <= c < dims
+ ensures
+ - Let M denote the matrix for this gate, then this function
+ returns a non-const reference to M(r,c)
+ !*/
+
+ template <typename exp>
+ qc_scalar_type compute_state_element (
+ const matrix_exp<exp>& reg,
+ long row_idx
+ ) const;
+ /*!
+ requires
+ - reg.nr() == dims
+ - reg.nc() == 1
+ - 0 <= row_idx < dims
+ ensures
+ - Let M represent the matrix for this gate, then this function
+ returns rowm(M*reg, row_idx)
+ (i.e. returns the row_idx row of what you get when you apply this
+ gate to the given column vector in reg)
+ !*/
+
+ static const long num_bits;
+ static const long dims;
+
+ };
+
+// ----------------------------------------------------------------------------------------
+
+ template <typename T, typename U>
+ const composite_gate<T,U> operator, (
+ const gate_exp<T>& lhs,
+ const gate_exp<U>& rhs
+ ) { return composite_gate<T,U>(lhs,rhs); }
+ /*!
+ ensures
+ - returns a composite_gate that represents the tensor product of the lhs
+ gate with the rhs gate.
+ !*/
+
+// ----------------------------------------------------------------------------------------
+
+ namespace quantum_gates
+ {
+
+ inline const gate<1> hadamard(
+ );
+ /*!
+ ensures
+ - returns the Hadamard gate.
+ (i.e. A gate with a matrix of
+ |1, 1|
+ 1/sqrt(2) * |1,-1| )
+ !*/
+
+ inline const gate<1> x(
+ );
+ /*!
+ ensures
+ - returns the not gate.
+ (i.e. A gate with a matrix of
+ |0, 1|
+ |1, 0| )
+ !*/
+
+ inline const gate<1> y(
+ );
+ /*!
+ ensures
+ - returns the y gate.
+ (i.e. A gate with a matrix of
+ |0,-i|
+ |i, 0| )
+ !*/
+
+ inline const gate<1> z(
+ );
+ /*!
+ ensures
+ - returns the z gate.
+ (i.e. A gate with a matrix of
+ |1, 0|
+ |0,-1| )
+ !*/
+
+ inline const gate<1> noop(
+ );
+ /*!
+ ensures
+ - returns the no-op or identity gate.
+ (i.e. A gate with a matrix of
+ |1, 0|
+ |0, 1| )
+ !*/
+
+ template <
+ int control_bit,
+ int target_bit
+ >
+ class cnot : public gate_exp<cnot<control_bit, target_bit> >
+ {
+ /*!
+ REQUIREMENTS ON control_bit AND target_bit
+ - control_bit != target_bit
+
+ WHAT THIS OBJECT REPRESENTS
+ This object represents the controlled-not quantum gate. It is a gate that
+ operates on abs(control_bit-target_bit)+1 qubits.
+
+ In terms of the computational basis vectors, this gate maps input
+ vectors to output vectors in the following way:
+ - if (the input vector corresponds to a state where the control_bit
+ qubit is 1) then
+ - this gate outputs the computational basis vector that
+ corresponds to the state where the target_bit has been flipped
+ with respect to the input vector
+ - else
+ - this gate outputs the input vector unmodified
+
+ !*/
+ };
+
+ template <
+ int control_bit1,
+ int control_bit2,
+ int target_bit
+ >
+ class toffoli : public gate_exp<toffoli<control_bit1, control_bit2, target_bit> >
+ {
+ /*!
+ REQUIREMENTS ON control_bit1, control_bit2, AND target_bit
+ - all the arguments denote different bits, i.e.:
+ - control_bit1 != target_bit
+ - control_bit2 != target_bit
+ - control_bit1 != control_bit2
+ - The target bit can't be in-between the control bits, i.e.:
+ - (control_bit1 < target_bit && control_bit2 < target_bit) ||
+ (control_bit1 > target_bit && control_bit2 > target_bit)
+
+ WHAT THIS OBJECT REPRESENTS
+ This object represents the toffoli variant of a controlled-not quantum gate.
+ It is a gate that operates on max(abs(control_bit2-target_bit),abs(control_bit1-target_bit))+1
+ qubits.
+
+ In terms of the computational basis vectors, this gate maps input
+ vectors to output vectors in the following way:
+ - if (the input vector corresponds to a state where the control_bit1 and
+ control_bit2 qubits are 1) then
+ - this gate outputs the computational basis vector that
+ corresponds to the state where the target_bit has been flipped
+ with respect to the input vector
+ - else
+ - this gate outputs the input vector unmodified
+
+ !*/
+ };
+
+ // ------------------------------------------------------------------------------------
+
+ }
+
+// ----------------------------------------------------------------------------------------
+
+}
+
+#endif // DLIB_QUANTUM_COMPUTINg_ABSTRACT_
+
+
+