A Note on Output Length of One-Way State Generators and EFIs
Pith reviewed 2026-05-24 05:40 UTC · model grok-4.3
The pith
There do not exist one-way state generators with O(log λ)-qubit outputs.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The central claim is that there do not exist OWSGs with O(log λ)-qubit outputs. This is shown by reducing any such short-output generator to a contradiction with the definition of one-wayness. Parallel results prove non-existence of O(log λ)-qubit EFIs while constructing ω(log λ)-qubit EFIs from exponentially secure PRGs, and give tight bounds for OWSG variants parameterized by their advantage ε.
What carries the argument
The standard OWSG security definition (a quantum polynomial-time adversary cannot recover the input with non-negligible probability from the output state) together with the fixed 2^m-dimensional Hilbert space of an m-qubit output register.
If this is right
- The Cavalar et al. construction with m=ω(log λ) is optimal for standard OWSGs.
- λ^{-c}-OWSGs require at least (c log λ - 2) qubit outputs.
- O(1)-advantage OWSGs require more than ((log log λ)/2) qubit outputs.
- Weak OWSGs ((1-1/poly(λ))-advantage) require ω(1) qubit outputs.
- EFIs cannot exist with O(log λ) qubit outputs.
Where Pith is reading between the lines
- The results suggest that quantum one-way primitives require output states with dimension growing faster than any polynomial in the security parameter to achieve negligible advantage.
- Designers of quantum protocols may need to allocate at least logarithmic qubit overhead when replacing classical one-way functions with state generators.
- The gap between the O(log log λ) constructions and the Ω(log log λ) lower bound for constant-advantage OWSGs leaves open whether the constants can be improved.
Load-bearing premise
That OWSG security is defined solely by the inability of a quantum polynomial-time adversary to recover the input with non-negligible probability from the output state.
What would settle it
An explicit construction of an OWSG whose outputs are O(log λ) qubits long and that meets the standard security definition against quantum polynomial-time adversaries.
read the original abstract
We study the output length of one-way state generators (OWSGs), their weaker variants, and EFIs. - Standard OWSGs. Recently, Cavalar et al. (arXiv:2312.08363) give OWSGs with $m$-qubit outputs for any $m=\omega(\log \lambda)$, where $\lambda$ is the security parameter, and conjecture that there do not exist OWSGs with $O(\log \log \lambda)$-qubit outputs. We prove their conjecture in a stronger manner by showing that there do not exist OWSGs with $O(\log \lambda)$-qubit outputs. This means that their construction is optimal in terms of output length. - Inverse-polynomial-advantage OWSGs. Let $\epsilon$-OWSGs be a parameterized variant of OWSGs where a quantum polynomial-time adversary's advantage is at most $\epsilon$. For any constant $c\in \mathbb{N}$, we construct $\lambda^{-c}$-OWSGs with $((c+1)\log \lambda+O(1))$-qubit outputs assuming the existence of OWFs. We show that this is almost tight by proving that there do not exist $\lambda^{-c}$-OWSGs with at most $(c\log \lambda-2)$-qubit outputs. - Constant-advantage OWSGs. For any constant $\epsilon>0$, we construct $\epsilon$-OWSGs with $O(\log \log \lambda)$-qubit outputs assuming the existence of subexponentially secure OWFs. We show that this is almost tight by proving that there do not exist $O(1)$-OWSGs with $((\log \log \lambda)/2+O(1))$-qubit outputs. - Weak OWSGs. We refer to $(1-1/\mathsf{poly}(\lambda))$-OWSGs as weak OWSGs. We construct weak OWSGs with $m$-qubit outputs for any $m=\omega(1)$ assuming the existence of exponentially secure OWFs with linear expansion. We show that this is tight by proving that there do not exist weak OWSGs with $O(1)$-qubit outputs. - EFIs. We show that there do not exist $O(\log \lambda)$-qubit EFIs. We show that this is tight by proving that there exist $\omega(\log \lambda)$-qubit EFIs assuming the existence of exponentially secure PRGs.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper proves lower bounds on output lengths for one-way state generators (OWSGs) and their variants (including ε-OWSGs, constant-advantage OWSGs, and weak OWSGs) as well as for EFIs. It shows non-existence of standard OWSGs with O(log λ)-qubit outputs (strengthening Cavalar et al.'s conjecture), provides almost-tight constructions from OWFs for weaker variants with specific output lengths like ((c+1)log λ + O(1)) for λ^{-c}-OWSGs, and establishes matching lower bounds; similar tightness results hold for EFIs assuming exponentially secure PRGs.
Significance. If the results hold, they establish optimality of known OWSG constructions in output length and resolve an open conjecture, while giving new constructions for parameterized/weak variants. The work strengthens the foundations of quantum cryptographic primitives by relating output size directly to security parameters and advantage levels.
major comments (2)
- [Abstract / main theorems on non-existence] Abstract and main non-existence claims: the proofs that no OWSGs exist with O(log λ)-qubit outputs (and analogous bounds for ε-OWSGs and constant-advantage OWSGs) reduce existence to a contradiction with one-wayness via a counting/search argument. This relies on modeling the output as an m-qubit register whose Hilbert space has dimension exactly 2^m. If the OWSG definition permits states supported on a strictly larger space (effective dimension not pinned to 2^m), the inversion advantage may become negligible and the non-existence result would not apply. Please state the precise definition of OWSG output used and confirm whether the argument extends to more general state spaces.
- [ε-OWSG results] Abstract, ε-OWSG section: the construction achieves ((c+1)log λ + O(1))-qubit outputs while the lower bound rules out at most (c log λ - 2) qubits. The O(1) additive gap is not closed; if the central claim is that the construction is 'almost tight,' the paper should either tighten the constants or explain why the gap cannot be removed under the same assumptions.
minor comments (2)
- [Preliminaries] Notation for output length m is used interchangeably with 'm-qubit outputs' without an explicit definition of the register dimension in the preliminaries; add a short paragraph clarifying the Hilbert-space modeling.
- [Weak OWSGs] The weak-OWSG construction assumes exponentially secure OWFs with linear expansion; cite the precise theorem or reference used for this assumption.
Simulated Author's Rebuttal
We thank the referee for the positive recommendation of minor revision and the detailed comments. We address each major comment below and will update the manuscript accordingly.
read point-by-point responses
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Referee: [Abstract / main theorems on non-existence] Abstract and main non-existence claims: the proofs that no OWSGs exist with O(log λ)-qubit outputs (and analogous bounds for ε-OWSGs and constant-advantage OWSGs) reduce existence to a contradiction with one-wayness via a counting/search argument. This relies on modeling the output as an m-qubit register whose Hilbert space has dimension exactly 2^m. If the OWSG definition permits states supported on a strictly larger space (effective dimension not pinned to 2^m), the inversion advantage may become negligible and the non-existence result would not apply. Please state the precise definition of OWSG output used and confirm whether the argument extends to more general state spaces.
Authors: We use the standard definition of an m-qubit OWSG, in which the output state resides in a Hilbert space of dimension exactly 2^m (i.e., the state is supported on an m-qubit register). This matches the definitions employed in Cavalar et al. and other prior works on OWSGs. The counting argument in our non-existence proofs explicitly uses the fact that there are at most 2^{2^m} distinct pure states in this space to obtain the contradiction with one-wayness. We will add a clarifying sentence in the preliminaries (and a footnote in the abstract) stating this precise definition. The argument does not apply to states whose effective support has dimension larger than 2^m, but such a relaxation falls outside the standard OWSG definition we consider. revision: yes
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Referee: [ε-OWSG results] Abstract, ε-OWSG section: the construction achieves ((c+1)log λ + O(1))-qubit outputs while the lower bound rules out at most (c log λ - 2) qubits. The O(1) additive gap is not closed; if the central claim is that the construction is 'almost tight,' the paper should either tighten the constants or explain why the gap cannot be removed under the same assumptions.
Authors: The leading coefficient c in both the construction ((c+1)log λ + O(1)) and the lower bound (c log λ - 2) matches exactly; the additive O(1) discrepancy is an artifact of the concrete security reductions (hybrid arguments and Chernoff bounds in the construction, and the precise counting thresholds in the lower bound). We view the bounds as almost tight because the dominant term is identical. Under plain OWFs it is unclear whether the additive constants can be fully closed without additional assumptions. In the revision we will insert a short paragraph after the ε-OWSG theorem statements explaining the source of the gap and reiterating that the results are asymptotically tight in the leading term. revision: yes
Circularity Check
No circularity: non-existence proofs rely on standard one-wayness definitions and dimension counting
full rationale
The paper proves non-existence of short-output OWSGs by reducing any candidate generator to a QPT adversary that inverts with non-negligible probability, using the standard definition of OWSG security and the modeling of outputs as m-qubit states (Hilbert space dimension 2^m). This reduction is external to the paper's own constructions or prior self-citations; it invokes no fitted parameters, self-definitional equations, or load-bearing self-citations. The cited conjecture of Cavalar et al. is treated as an external statement being strengthened, not as an internal premise. All bounds follow directly from counting arguments on the output register without renaming or smuggling ansatzes. The derivation is therefore self-contained against the standard cryptographic definitions.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Existence of (subexponentially secure) one-way functions or pseudorandom generators with linear expansion.
- standard math Standard definition of quantum polynomial-time adversaries and negligible vs. inverse-polynomial advantage.
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