nLab quantum circuits via dependent linear types

Quantum circuits via dependent linear types

under construction


Quantum systems

quantum logic

quantum physics

quantum probability theoryobservables and states

quantum information

quantum computation

quantum algorithms:


Quantum circuits via dependent linear types


The problem

In the context of quantum computation, a pure quantum circuit diagram (originally: “quantum computational network”, Deutsch 1989) is a kind of string diagram (Abramsky & Coecke 2004) in finite-dimensional Hilbert spaces, typically used to express a sequence of low-level quantum gates mapping between spaces of pure quantum states.

A generic pure quantum circuit might look as follows:

Here, for instance, the “quantum gateU 34U_{34} is a linear operator on the tensor product Hilbert space \mathscr{H} \oplus \mathscr{H}.

Notice that the quantum circuit is understood to be the actual string diagram, up to the usual admissible topological deformations, not just the composite linear transformation which it encodes: The compositeness of the diagram encodes how (e.g. in which order) available quantum gate-operations would be operated on an actual quantum computer, and the composite linear map only encodes the inpute-to-output-specification of the resulting quantum computation. In this sense, quantum circuits constitute a quantum programming language and one also speaks of the “quantum circuit model of quantum computation” (e.g. Nielsen & Chuang 2000, §II.4.6; Miszczak 2011, §3, 2012, §4.3; Beneti & Casati 2018, §3.2).

Often the basic Hilbert space building block here is taken to be complex 2-dimensional, 2\mathscr{H} \,\coloneqq\, \mathbb{C}^2, in which case one speaks of a quantum circuit on q-bits.

Typically all quantum gates involved, and hence also the resulting composite linear maps, are assumed to be invertible, as befits reversible computation by unitary quantum state evolution in quantum mechanics.

But more generally and certainly in the broader context of quantum information theory (such as in formulating the quantum teleportation protocol and similar), quantum circuits are admitted to cross the quantum-classical divide?, in that they may involve:

  1. quantum measurement,

  2. quantum state preparation,

  3. classically controlled quantum gates.

All three of these appear already in basic examples such as the quantum teleportation protocol:

Yet more generally — notably for any plausible implementation of quantum error correction — one needs to allow for quantum measurement-results to be fed back during runtime (“dynamic lifting”) into algorithms running on a universal classical computer which schedule further quantum circuit-execution, and so forth:

SQRAM model adapted from Nagarajan, Papanikolaou Williams 2007, Fig 1

The conceptual subtlety with fully formalizing these common ideas is that quantum measurement, in particular, is not only non-reversible (due to the quantum state collapse involved) but also non-deterministic, meaning that it is not immediately represented by a fixed linear map at all – at least not between the original Hilbert spaces.

Concretely, the “projection postulate” of quantum physics asserts (von Neumann 1932; Lüders 1951) that:

  1. measurement of quantum states is with respect to a choice of orthonormal linear basis {|ψ b} b:B\big\{\vert \psi_b \rangle \big\}_{b : B} of the given Hilbert space \mathscr{H} of pure quantum states;

  2. the result of measurement on pure quantum states |ψ\vert \psi \rangle \;\in\; \mathscr{H} is

    1. a random value bBb \in B;

    2. the “collapse” of the quantum state being measured by orthogonal projection to the the linear span of the bbth basis state.

      P b : B |ψ P b|ψ=|ψ bψ b|ψ \array{ P_b &\colon& \mathscr{H} &\xrightarrow{\phantom{---}}& \mathscr{H}_B \hookrightarrow \mathscr{H} \\ && \vert \psi \rangle &\mapsto& P_b \vert \psi \rangle \mathrlap{ = \vert \psi_b \rangle \langle \psi_b \vert \psi \rangle } }

There are different ways to type the quantum measurement, taking into account the non-deterministic nature of its outcome:

  1. Regarding the direct sum b:B\bigoplus_{b \colon B} \mathscr{H} of Hilbert spaces as the logical disjunction (“or”) of quantum logic, one may regard measurement as being the linear map into the direct sum whose bbth component is P bP_b.

    This choice of typing appears (briefly) in Selinger 2004, p. 39, in a precursor discussion that led to the formulation of the quantum programming language Quipper.

  2. Regarding the measurement outcome bBb \in B as the observed context of the actual quantum collapse, one may regard the collapse projection as dependently typed.

    Getting from previous option back to this one is known in the the Quipper-community as dynamic lifting (namely “of the measured bits back into the context”)

Both of these options naturally emerge and are naturally unified in the “Quantum Modal Logic” inherent to dependent linear type theory: This is what we now discuss.

A solution

The following discussion indicates1 how a natural quantum programming language for quantum information-processing protocols — hence for quantum circuits consisting of general quantum gates with classical control, including de-coherent quantum measurement-gates and subsequent coherent quantum gates depending on these — is elegantly subsumed within any dependent linearly typed programming language which expresses the “yoga of six operations”, such as is the case in the linear homotopy type theory of Riley 2022.

This works by regarding classically controlled quantum states as having linear data types dependent on classical control parameters and on measurement results, and then making the following key observations on modal quantum logic with dependent linear types:

  1. The “necessitymodality C(p C) *(p C) *\Box_C \coloneqq (p_C)^\ast (p_C)_\ast on linear types dependent on a given classical context CC (which includes classical control parameters as well as eventual quantum measurement-outcomes on the same footing) knows all about controlled quantum gates: These are identified just with the morphisms of the C\Box_C-co-Kleisli category, where the C\Box_C-counit (taking a linear type “out of the comonad”) reflects the quantum state collapse of quantum measurement, and where the C\Box_C-comultiplication encodes the superposition-principle.

  2. The external tensor product of dependent linear types gives the compilation of quantum gates into quantum circuits, essentially as familiar from the quantum string diagram-calculus of Abramsky & Coecke 2004 with respect to the plain tensor product, but now taking into account dependency on classical control and potential measurement outcomes.

All constructions and proofs here flow readily from just the six operation yoga and (co-)Kleisli theory. One key point is (4) that the necessity modality respects the external tensor product – so that these classically controlled quantum circuits are unambiguously defined –, under the assumption that it coincides with the dual possibility modality C C\lozenge_C \mathscr{H}_C on the quantum data types \mathcal{H}_\bullet involved – hence (in full generality) when the linear types are dualizable in the sense of ambidexterity and specifically (in the traditional models) when quantum state spaces are finite dimensional, as is the case in quantum information theory.

Aspects of the following have a resemblance to some variants and categorical interpretations of the quantum programming languageQuipper” (see the references there), but avoids (see below) Quipper’s problem of needing “dynamic lifting” (see there) of “measurement bits back into the context”: The linear necessity-modality knows right away that measurement outcomes are recorded in the context.

Idea: Modal quantum logic via linear homotopy types

We assume a dependent linear type theory which functorially obtains (as anticipated in Schreiber 2014, §3.2 and established in Riley 2022, §2.4):

  1. from a classical (“intuitionistic”) type X:TypeX : Type a (large) type LinType XLinType_X of linear types dependent on XX, equipped with symmetric closed monoidal structure ()()(-) \otimes (-) (tensor product) and [,][-,\,-] (internal hom);

  2. from a function f:X 1X 2f : X_1 \xrightarrow{\;} X_2 between classical types a yoga of six operations (specifically: a “Wirthmüller context”) between their types of dependent linear types, hence a contravariant substitution/pullback operation f *f^\ast which is strong monoidal, strong closed and extends to a base change adjoint triple (with left adjoint f !f_! a version of dependent sum and right adjoint a version of dependent product):

Classical modal logic

First observe that (without imposing a further condition) also classical (“non-linear”) dependent type theory provides an example of this yoga of six operations (actually five distinct operations, in the present case of Wirthmüller contexts), with:

  1. tensor product given by product types,

  2. internal hom given by function types,

  3. f *f^\ast given by context extension,

  4. f !f_! given by dependent coproduct,

  5. f *f_\ast given by dependent product.

In this classical situation, the (co-)monad adjoint pair C C\lozenge_C \dashv \Box_C induced by the adjoint triple is readily found (see here) to reflect the necessity-modality and the possibility-modality of a kind of modal logic which regards the potential measurement outcomes c:Cc : C as “possible worlds”:

In fact there is (see here) a quadruple of (co-)monadic modalities associated with any base change:


  1. the definiteness-modality \star is also known as the writer comonad;

  2. the randomness-modality \bigcirc is also known as the reader monad.

We recover the meaning of these expressions in terms of quantum measurement and quantum state preparation, below.

(In general there may be richer dependency on classical contexts. In the next simplest case the base change is along the projection map out of a Cartesian product of classical types, which makes one of them label potential upcoming measurement results as before, while the other encodes further dependency on classical parameters, such as on previous measurement results:

This plays a role for classically-controlled quantum gates, below).

Quantum modal logic

This general modal logic of possible worlds found inside dependent type theory becomes subject to one curious further rule as we pass to genuinely linear types, such as in the sense of stable homotopy types in linear homotopy type theory:

Namely, assuming that the potential measurement outcomes c:Cc \colon C form a finite set — which is the case of relevance in quantum information theory —, the linearity or stability axiom implies that the base change down from the context CC becomes ambidextrous, in that on dependent linear types \mathscr{H}_\bullet the coproduct computed by the possibility-modality and the product computed by the necessity-modality agree (the situation of a “biproduct”):

BC:FinSet, :LinType B . BC : FinSet ,\;\; \mathscr{H}_\bullet \,\colon\, LinType_B \;\;\;\;\; \vdash \;\;\;\;\; \lozenge \mathscr{H}_\bullet \;\simeq\; \Box \mathscr{H}_\bullet \,.

Curiously, in terms of modal logic, this is the Gell-Mann principle of quantum physics:

Thepossible is necessary and hence actualized ϵ with some probability \array{ \llap{\text{The}}\;\text{possible} & \text{is} & \text{necessary} & \text{and hence} & \text{actualized} \\ \lozenge \mathcal{H}_\bullet & \simeq & \Box \mathcal{H}_\bullet & \xrightarrow{\phantom{--} \epsilon \phantom{--}} & \mathcal{H}_{ \bullet \; \mathrlap{\text{with some probability}} } }

Concretely, the linear homotopy type theory of Riley 2022 should have categorical semantics in the \infty -topos of parameterized H H\mathbb{C} -module spectra (S. 2014, Ex. 3.11) and complex vector spaces embed into this stable homotopy theory under passage to their Eilenberg-MacLane spectra (see the stable Dold-Kan correspondence).

(1)It is convenient and meaningful to declare the notational conventions to: \text{It is convenient and meaningful to declare the notational conventions to:} \phantom{--------------------}
  1. abbreviate p ! p * \mathscr{H} \,\coloneqq\, p_! \mathscr{H}_\bullet \,\simeq\, p_\ast \mathscr{H}_\bullet

  2. notationally suppress any outer application of (p B) *:LinTypeLinType B(p_B)^\ast \colon LinType \to LinType_B;

Thereby, the definiteness/randomness modalities in relation to necessity and possibility of classical modal logic (above) may be expressed in quantum modal logic by:

This way, the default categorical semantics for modal quantum logic is that of bundles of finite dimensional vector spaces (finite-dimensional complex Hilbert spaces) over finite sets: In this case both (p C) !(p_C)_! as well as (p C) *(p_C)_\ast yield the ordinary direct sum of the fibers (a biproduct). Since this is the categorical semantics under which the following type theory describes the traditional quantum circuits, we will adopt our notation to this case and denote the generic dependent linear type by :LinType C\mathcal{H}_\bullet : LinType_C and its generic term by the usual notation for quantum states:

c:C|ψ c: c. c : C \;\;\; \vdash \;\;\; \vert \psi_c \rangle \;\colon\; \mathcal{H}_c \,.

one finds for the base change adjoint triple of dependent linear types along finite fibers (?) that the interpretation of their (co-)units is as follows:

By the assumption that BB is finite and since Vect has biproducts, the colimit/coproduct

(p B) !𝒱 = b:B𝒱 b (p_B)_! \mathscr{V}_\bullet \;=\; \coprod_{b : B} \mathscr{V}_b

and the limit/product

(p B) *𝒱 = b:B𝒱 b (p_B)_\ast \mathscr{V}_\bullet \;=\; \prod_{b : B} \mathscr{V}_b

agree (we have an ambidextrous adjunction) and are both equivalent to the direct sum:

(p B) !𝒱 (p B) *𝒱 =b:B𝒱 b. (p_B)_! \mathscr{V}_\bullet \;\simeq\; (p_B)_\ast \mathscr{V}_\bullet \;=\; \underset{b \colon B}{\bigoplus} \mathcal{V}_b \,.

Accordingly, the underlying endofunctors of the induced monad and comonad on kVec Bk Vec_B

B(p B) *(p B) * B(p B) *(p B) !:kVec BkVec B \Box_B \;\coloneqq\; (p_B)^\ast (p_B)_\ast \;\;\vdash\;\; \lozenge_B \;\coloneqq\; (p_B)^\ast (p_B)_! \;\;\colon\;\; k Vec_B \longrightarrow k Vec_B

agree, to make a self-adjoint functor

(p B) * B(p B) * B:kVeckVec (p_B)^\ast \bigotimes_B \;\;\vdash\;\; (p_B)^\ast \bigotimes_B \;\;\;\colon\;\;\; k Vec \longrightarrow k Vec

which carries the structure both of a monad and of a comonad.

This way, one finds that the four (co)unit operations of quantum modal logic are given as follows:


Quantum modality

In addition to the above schemata of (co)monads acting on the (dependent) linear type systems, we invoke the relative monad

Q : Type LType B B𝟙 \array{ \mathrm{Q} &\colon& Type &\longrightarrow& LType \\ && B &\mapsto& \underset{B}{\bigoplus} \mathbb{1} }

which sends a finite type (in particular) to the direct sum that it spans (a detailed description of this relative monad is here).

This is in fact idempotent, in that the actual monad on the full dependent linear type system that this relative monad is induced by is the idempotent monad which witnesses a reflective subcategory-inclusion of the linear types into dependent linear types:

Q:Type()×𝟙DLTypeLTypeDLType. \mathrm{Q} \;\colon\; Type \xrightarrow{ (-) \times \mathbb{1} } DLType \twoheadrightarrow LType \xhookrightarrow{ \phantom{---} } DLType \,.

This implies that whenever D:LTypeD \;\colon\; LType, we may describe morphisms of the form QBLType\mathrm{Q}B \to LType by Kleisli morphisms for Q\mathrm{Q}.

For example for B=BitB = Bit the type of classical bits, we have that

Q(Bit)=QBit \mathrm{Q}(Bit) \;=\; QBit

is the usual type of q-bits.

Quantum gates

The morphisms in the (co-)Kleisli category of \Box and \bigcirc are linear maps

= = \mathscr{H} \;=\; \Box \mathscr{H}_\bullet \xrightarrow{\;} \bigcirc \mathscr{H}_\bullet \;=\; \mathscr{H}

in the image of p B *p_B^\ast and as such are quantum gates (we show how to restrict these to unitary operators below in …).

Inspection shows that the four ways of relating these to (co-)Kleisli morphisms correspond to composing quantum gates with:

  1. quantum measurement

  2. quantum state preparation

  3. quantum superposition

  4. quantum parallelization:

Quantum measurement

Specifically, C\Box_C-actualization is the measurement process – in that the C\Box_C-counit implements exactly the rule for wavefunction collapse (due to Lüders 1951, following von Neumann 1932, §III.3 and §VI) with regards to quantum measurements in the CC-indexed basis of the total Hilbert space C \mathcal{H} \coloneqq \Box_C \mathcal{H}_\bullet which is encoded by its direct sum decomposition \mathcal{H}_\bullet:

Given this, the Kleisli equivalence for the necessity comonad B\Box_B is essentially the deferred measurement principle for quantum circuits:

We may understand quantum measurement in this form as the effect handling (in the sense of monads in computer science) of indefiniteness effects (in the sense of potentiality modal logic):

Notice that this process may be understood as the “dynamic lifting” of quantum measurement-results into the context (here: B=B = Bool) of the ambient dependent linear type theory.

There is another possible typing of quantum measurement, where a measurement lands in the random reader monad:

These two are related by the following diagram commutes (being the naturality square of the necessity-counit on the possibility-unit):


In the bottom row are making use of the notation (1).

Quantum circuits

While quantum gates have horizontal composition in the co-Kleisli category, they also have a vertical composition given by external tensor product:

The point here is that the external tensor product records not just the tensor product on the given linear/quantum types, but also the fact that under combining two quantum gates/circuits, the types CC and CC' of their potential classical measurement outcomes combine into the type C×CC \times C' of pairs of outcomes (the Cartesian product) — see the example of pairs of qbits, below.

One checks that for ambidextrous/finite-dimensional dependent linear types, the necessity-modality respects the external tensor product:

(4) C×C( )(( C )( C )) \Box_{C \times C'} \big( \mathscr{H}_\bullet \boxtimes \mathscr{H}'_\bullet \big) \;\simeq\; \Big( \big( \Box_{C} \mathscr{H}_\bullet \big) \boxtimes \big( \Box_{C '} \mathscr{H}'_\bullet \big) \Big)

This implies that well-defined quantum circuits may be compiled from iterating between

  1. horizontally composing morphisms in the co-Kleisli category of a necessity-modality applicable to given quantum types;

  2. vertically adjoining such morphisms via their external tensor product.

We illustrate below how this provides a (programming) language for all tranditional quantum circuits compiled from qbits.

But the expressiveness of the ambient linear homotopy type theory is considerably larger and allows to handle more general notions of quantum circuits with the same language structures. For instance:

  1. We may use (in fact: construct) quantum types as building blocks which are not just qbits but much richer spaces of conformal blocks (SS22). This allows to natively compile quantum programs for anyon braid gates as used in topological quantum computation.

  2. Instead of just (parameterized) complex vector spaces, the language of linear homotopy type theory in Riley 2022 handles more general (parameterized) H H\mathbb{C} -module spectra, and in fact (parameterized) RR-module spectra over any E E_\infty -ring spectrum RR.

(A first example of quantum gates operating on spectra appears in the above-mentioned construction of conformal block if one just omits the fiberwise 0-truncation in the last step.)

Example: Traditional QBit-based quantum circuits

We spell out in terms of the above modal quantum logic found inside dependent linear type theory the traditional zoo of quantum gates and basic quantum circuits acting on tensor products of qbits. On the one hand this serves to show how all the expected constructions are naturally recovered, on the other hand it enhances these standard concepts by what is de-facto a quantum programming language for their classically-controlled versions (as such somewhat akin to parts of Quipper, but avoiding the issue of “dynamic lifting”, see below).

To start with, a moment of reflection reveals that the linear type of a single (in-)coherent qbit is as follows, depending on the classical type of booleans (which here we denote by “0” and “1” instead of “false” and “true”) .

The quantum measurement-process on such a qbit type, as seen by the necessity-counit, verifies the projection postulate of measurements in quantum mechanics:

Notice that one might be tempted2 to think of this formula as outputting the classical bit b:Boolb : \mathrm{Bool}, but that the dependent typing of the above expression is a little more subtle than that: The output bit is instead part of the context inside which the collapsed wavefunction qbit appears – which, being in the 1-dimensional Hilbert space \mathbb{C} in this case, may often be disregarded as a global phase, but is nevertheless the actual output of the measurement process.

In particular, by retaining the quantum type of the measurement result, we retain the ability to speak about repeated quantum measurement, which leads to a proof that the second measurement necessarily gives the same result as the first (the experimental observation of this fact is what originally led to the formulation of the projection postulate, in von Neumann 1932, §III.3):

In the other (vertical) direction, the dependent linear type of the measurement of a pair of qbits comes out as expected, where the point to notice is how the external tensor product keeps track of the fact that a pair of qbits has 2×2=42 \times 2 = 4 potential measurement outcomes:

Dually, the possibility-unit on qbits is their conditional state preparation (this is the operation denoted “a̲a\underline{a} \xleftarrow{\;} a” in Knill 1996, p. 8):

From this, if we denote const 0:BoolBool\mathrm{const}_0 \colon \Bool \to \Bool the function constant on 00, then the unconditional state preparation (the operation denoted “a̲0\underline{a} \xleftarrow{\;} 0” in Knill 1996, p. 8) is the base change of the conditional state preparation along this map:

The dependent linear type of the Hadamard gate:

The dependent linear type of the CNOT gate:

The dependent linear type of a Bell state preparation:

The dependent linear type of a Bell state measurement:

The dependent linear type of a quantum gate controlled by a classical bit:

This establishes all the ingredients of traditional quantum circuits. For instance, we obtain the measurement-controlled circuit that exhibits the quantum teleportation-protocol:


Quantum Programming Language

With all elements of quantum circuits formulated via (co)monads constructed inside a language of dependent linear types as above, we obtain an embedded quantum programming language for quantum circuits with classical control and effects.

Quantum/classical types and modalities

We use the following notation for the type system and the quantum/classical modalities on these.

Here the expressions in square brackets may be thought of as the corresponding categorical semantics as bundles of linear types (for instance semantics in the category VectBund of complex vector bundles over Sets, or more generally, in the \infty -category of parametrized H H\mathbb{C} -module spectra).

The classical modality \natural and the quantum modality Q\mathrm{Q} send a bundle type to its base and to its “linearized total space”, respectively:

(The quantum monad Q\mathrm{Q} is a relative monad; its categorical semantics in VectBund is discussed there.)

The classical internal hom and its quantum version relative to the (“external”) linear tensor product (for more on this see the discussion here at VectBund):

Notice that all these types are bundles “in themselves”, in that we did not invoke (yet) any dependent types (semantically we speak about a total tangent \infty -topos, not its system of slice \infty -categories).

Instead, the actual BB-dependent types that we need to reflect (“dynamic lifting” of) quantum measurement will all be viewed, indirectly, through the lens of B\bigcirc_B-modales on the non-dependent types (view the comparison functor which here is an equivalence).

The only explicit context that we do need to consider is – besides the trivial dependency on the classical unit type *\ast, its quantum analog namely: – dependency on the tensor unit 𝟙\mathbb{1}. This only exception to the rule we sugar away by the following “circle-colon”-notation (which is meant to rhyme on the “\multimap”-notation for linear implication):

Sugaring modal dependent linear types to a quantum language

We now obtain a quantum programming language from modal dependent linear type theory simply by meticulously sugaring:

(1) the standard do-notation for monads in computer science,

(2) the (co)pure/return-functions of the various monads.

Syntax for effect binding

We code maps in the Kleisli category of an effect monad \mathcal{E} by this schema:

This syntax is to closely reflect the fact that

  • for an input of the form return D (d):D\return^{\mathcal{E}}_D(d) \colon \mathcal{E}D

  • which may appear as a contribution in the effectful input data,

  • the operation bind prog \bind^{\mathcal{E}}_{\mathrm{prog}} does produce the output prog(d)\mathrm{prog}(d),

which prescription completely defines it.


Beware that common classical notation for exactly the same costruction is a little different:

This classical notation is meant to suggest that pure data d:Dd \colon D may be “read out” from effectful data e:De \colon \mathcal{E}D. While this is suggestive for the list monad and its common relatives in classical programming, it is misleading in linear type theory and notably so for the quantum monad Q\mathrm{Q}: Here the effectful input e=|ψe = \vert \psi \rangle is a quantum state like a q-bit, in which case d:Bitd \colon Bit is a classical bit, whence the classical notation “d|ψd \leftarrow \vert \psi \rangle” could only be suggestive of performing a quantum measurement – in contradiction to the actual nature of the resulting bind prog Q\bind^{\mathrm{Q}}_{\mathrm{prog}}-operation constituting a coherent non-measurement quantum gate.

Instead, what really happens in Kleisli formalism is that operations are defined on generators for effectful data types (D)\mathcal{E}(D), namely on data of the form return D (d)\return^{\mathcal{E}}_D(d). For example, the space of qbits |ψ:QBit\vert \psi \rangle \colon \QBit is generated (here: linearly spanned) by the basis qbits |0\vert 0 \rangle and |1\vert 1 \rangle, where we may naturally identify the ket-notation |\vert - \rangle as the unit/return operation which regards a classical bit bb as the corresponding basis quantum state |b\vert b \rangle.

Moreover, we write an analogous for maps out of tensor products, using that these are generated from the homogeneous tensor products.


Syntax for pure effects

Finally, the monad-return operations`return` ()`return`^{\mathcal{E}}(-)” (and the comonad extract operations) we sugar according to the following table:

In the same vein we sugar the constructor for terms in the quantum reader monad B\bigcirc_B as follows:

Example pseudo-code

Basic qbit circuit ingredients

Basic quantum logic gates on qbits:

The quantum NOT/Pauli X-gate

The Hadamard gate:

The CNOT gate:

Quantum teleportation protocol

The quantum teleportation protocol:

is given by the following code:

Quantum bit flip code

The quantum bit flip code for 3-qbit encoding:


The above figure of an SQRAM scheme is taken from:

  • Rajagopal Nagarajan, Nikolaos Papanikolaou, David Williams, Simulating and Compiling Code for the Sequential Quantum Random Access Machine, Electronic Notes in Theoretical Computer Science Volume 170, 6 March 2007, Pages 101-124 [doi:10.1016/j.entcs.2006.12.014]


  1. Full details to appear at: Topological Quantum Programming in Linear Homotopy Type Theory.

  2. Indeed, in Quipper the measurement process on a qbit is originally typed as “QBitBit\QBit \to \Bit” and further language design is needed to “bring the output bit back into the context”, see references on “dynamic lifting”.

Last revised on November 26, 2022 at 09:54:14. See the history of this page for a list of all contributions to it.