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author | Daniel Baumann <daniel.baumann@progress-linux.org> | 2024-03-09 13:19:48 +0000 |
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committer | Daniel Baumann <daniel.baumann@progress-linux.org> | 2024-03-09 13:20:02 +0000 |
commit | 58daab21cd043e1dc37024a7f99b396788372918 (patch) | |
tree | 96771e43bb69f7c1c2b0b4f7374cb74d7866d0cb /ml/dlib/dlib/quantum_computing/quantum_computing_abstract.h | |
parent | Releasing debian version 1.43.2-1. (diff) | |
download | netdata-58daab21cd043e1dc37024a7f99b396788372918.tar.xz netdata-58daab21cd043e1dc37024a7f99b396788372918.zip |
Merging upstream version 1.44.3.
Signed-off-by: Daniel Baumann <daniel.baumann@progress-linux.org>
Diffstat (limited to 'ml/dlib/dlib/quantum_computing/quantum_computing_abstract.h')
-rw-r--r-- | ml/dlib/dlib/quantum_computing/quantum_computing_abstract.h | 590 |
1 files changed, 590 insertions, 0 deletions
diff --git a/ml/dlib/dlib/quantum_computing/quantum_computing_abstract.h b/ml/dlib/dlib/quantum_computing/quantum_computing_abstract.h new file mode 100644 index 000000000..bcc65af23 --- /dev/null +++ b/ml/dlib/dlib/quantum_computing/quantum_computing_abstract.h @@ -0,0 +1,590 @@ +// 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_ + + + |