Radial Fast Entangling Gates Under Micromotion in Trapped-Ion Quantum Computers
Pith reviewed 2026-05-17 21:18 UTC · model grok-4.3
The pith
Micromotion can be used to design high-fidelity entangling gates on radial modes in hundreds of nanoseconds.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
By incorporating the deterministic micromotion into quantum control frameworks, high-fidelity entangling gates can be realized on the radial modes of a two-ion crystal, with operation times ranging from hundreds of nanoseconds to microseconds and particularly effective in the sub-trap-period regime.
What carries the argument
Control sequences designed to include and exploit micromotion in the radial modes of a two-ion crystal.
If this is right
- High-fidelity entangling gates become feasible at timescales of hundreds of nanoseconds using radial modes.
- The physical origin of the micromotion benefit is identified through analysis of the control solutions.
- Gate error remains manageable when laser intensity fluctuations, trap-voltage noise, and positioning errors are included at laboratory levels.
- Radial modes, previously avoided due to micromotion, can now support fast operations.
Where Pith is reading between the lines
- The same incorporation of micromotion could be tested on chains with more than two ions to check scalability.
- Trap designs that deliberately engineer rather than suppress micromotion might become advantageous.
- Direct experimental comparison of these radial gates with conventional axial-mode gates would quantify the speed advantage.
Load-bearing premise
Micromotion can be modeled accurately enough that the resulting control sequences stay robust when real laboratory imperfections such as laser fluctuations and trap voltage noise are added.
What would settle it
An experiment that applies one of the identified sequences to radial modes and measures whether the achieved gate fidelity matches the predicted high value or falls well below it under typical lab noise.
Figures
read the original abstract
Micromotion in radio-frequency ion traps is generally considered detrimental for quantum logic gates, and is typically minimized in state-of-the-art experiments. However, as a deterministic effect, it can be incorporated into quantum control frameworks aimed at designing high-fidelity quantum logic controls. In this work, we demonstrate that micromotion can be beneficial to the design of fast gates utilizing the radial modes of a two-ion crystal, particularly in the sub-trap-period regime where high-fidelity control sequences are identified with operation times ranging from hundreds of nanoseconds to microseconds. Through analysis of select fast gate solutions, we uncover the physical origin of micromotion enhancement and further study the induced gate error under experimental noises and control imperfections. This analysis establishes the feasibility of realising high-fidelity entangling gates in hundreds of nanoseconds using the micromotion-sensitive radial modes of trapped-ion crystals.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript presents a quantum control framework that incorporates the deterministic micromotion effect in radio-frequency ion traps to design high-fidelity fast entangling gates utilizing the radial modes of a two-ion crystal. High-fidelity control sequences are identified for operation times ranging from hundreds of nanoseconds to microseconds in the sub-trap-period regime. The authors analyze the physical origin of the micromotion-induced enhancement and evaluate the resulting gate errors under experimental noises and control imperfections, thereby establishing the feasibility of realizing such gates on short timescales.
Significance. If the results hold, this work is significant for trapped-ion quantum computing because it demonstrates how a typically minimized effect can be turned into an advantage for achieving entangling gates substantially faster than the trap period. Faster gates reduce exposure to decoherence and support deeper circuits in scaled systems. The error analysis under realistic noises adds practical value, and the identification of specific sequences with physical insight strengthens the contribution.
major comments (2)
- [§5] §5, noise robustness analysis: While gate errors are studied for individual experimental imperfections (laser intensity fluctuations, trap-voltage noise, positioning errors), the manuscript does not quantify the fidelity when these imperfections act simultaneously at realistic laboratory amplitudes over the short gate duration. This combined robustness is load-bearing for the central feasibility claim.
- [§4.2, Eq. (12)] §4.2, Eq. (12): The effective radial-mode coupling under micromotion is derived from the time-dependent Hamiltonian, but the step showing how the deterministic micromotion term produces the reported enhancement (without additional free parameters) is not fully expanded; a explicit expansion of the interaction-picture terms would confirm the origin of the benefit.
minor comments (2)
- [Figure 3] Figure 3 caption: The noise amplitudes and simulation parameters used for the error plots should be stated explicitly to allow direct comparison with experimental conditions.
- [Introduction] Introduction: Adding a brief reference to recent experimental demonstrations of radial-mode gates would better situate the novelty of the micromotion-assisted approach.
Simulated Author's Rebuttal
We thank the referee for their positive summary and for highlighting the potential significance of our results on micromotion-enhanced fast radial gates. We address each major comment below and will revise the manuscript to strengthen the presentation and analysis.
read point-by-point responses
-
Referee: §5, noise robustness analysis: While gate errors are studied for individual experimental imperfections (laser intensity fluctuations, trap-voltage noise, positioning errors), the manuscript does not quantify the fidelity when these imperfections act simultaneously at realistic laboratory amplitudes over the short gate duration. This combined robustness is load-bearing for the central feasibility claim.
Authors: We agree that simultaneous noise sources represent an important practical consideration for the feasibility of sub-trap-period gates. In the revised manuscript we will add a combined-error analysis in §5, using Monte Carlo sampling over realistic laboratory amplitudes of laser intensity fluctuations, trap-voltage noise, and positioning errors to report the resulting fidelity distribution for the identified fast-gate solutions. revision: yes
-
Referee: §4.2, Eq. (12): The effective radial-mode coupling under micromotion is derived from the time-dependent Hamiltonian, but the step showing how the deterministic micromotion term produces the reported enhancement (without additional free parameters) is not fully expanded; a explicit expansion of the interaction-picture terms would confirm the origin of the benefit.
Authors: We appreciate the suggestion to make the derivation more transparent. In the revised version of §4.2 we will insert an explicit, step-by-step expansion of the interaction-picture Hamiltonian, isolating the contributions from the deterministic micromotion term and showing how they generate the effective coupling reported in Eq. (12) without additional free parameters. revision: yes
Circularity Check
No significant circularity; derivation uses standard Hamiltonians plus deterministic micromotion term
full rationale
The paper augments the usual trapped-ion Hamiltonian with a known deterministic micromotion term, then numerically identifies fast control sequences on the radial modes and analyzes their fidelity under added noise. No quoted step reduces a claimed prediction or uniqueness result to a fit performed on the same data, a self-citation chain, or a redefinition of the target quantity. The reported gate times and fidelities are outputs of the model rather than inputs, and the noise study is performed on the forward-simulated dynamics. This is the normal, non-circular case for a quantum-control design paper.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption The micromotion in an RF Paul trap is a deterministic, known function of the trap parameters and can be included exactly in the time-dependent Hamiltonian.
Lean theorems connected to this paper
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
We employ the Generalised Pulse Group (GPG) scheme... to find high-fidelity gate solutions... Eqs. (18a–c) for Θ, ΔXα, ΔYα with micromotion tensors μ(c,s), κ(c,s).
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
mode functions uα(t) solving the Mathieu-Hill equation... secular frequency ωα ≡ βα ΩRF/2
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
and motional restoration (∆X α = ∆Yα = 0 for each mode). As a result, the exact sequence of SDK timings and magnitudes that constitute a fast gate scheme must be found via numerical minimisation of Eq. (23). Optimisation over the unconstrained 2N-dimensional parameter space is numerically intractable, and thus constraints must be placed on the SDK sequenc...
-
[2]
The former case corresponds to a region in Fig. 2(a) where micromotion-enhanced fidelities are observed, and the latter case is an example of where high-fidelity solutions can be found for all micromotion amplitudes. Fig. 4(a) shows that, for gate speeds comparable or faster than a trapping period, accessing the regime of micromotion-enhanced gate fidelit...
-
[3]
J. I. Cirac and P. Zoller, Physical Review Letters74, 4091 (1995)
work page 1995
-
[4]
C. D. Bruzewicz, J. Chiaverini, R. McConnell, and J. M. Sage, Applied Physics Reviews6, 021314 (2019), https://pubs.aip.org/aip/apr/article-pdf/doi/10.1063/1.5088164/19742554/021314\ 1\ online.pdf
- [5]
-
[6]
L. J. Stephenson, D. P. Nadlinger, B. C. Nichol, S. An, P. Drmota, T. G. Ballance, K. Thirumalai, J. F. Goodwin, D. M. Lucas, and C. J. Ballance, Phys. Rev. Lett.124, 110501 (2020)
work page 2020
- [7]
-
[8]
J. O’Reilly, G. Toh, I. Goetting, S. Saha, M. Shalaev, A. L. Carter, A. Risinger, A. Kalakuntla, T. Li, A. Verma, and C. Monroe, Phys. Rev. Lett.133, 090802 (2024)
work page 2024
-
[9]
M. C. Marshall, D. A. R. Castillo, W. J. Arthur-Dworschack, A. Aeppli, K. Kim, D. Lee, W. Warfield, J. Hinrichs, N. V. Nardelli, T. M. Fortier, J. Ye, D. R. Leibrandt, and D. B. Hume, Phys. Rev. Lett.135, 033201 (2025)
work page 2025
-
[10]
B. C. Nichol, R. Srinivas, D. P. Nadlinger, P. Drmota, D. Main, G. Araneda, C. J. Ballance, and D. M. Lucas, Nature 609, 689 (2022)
work page 2022
-
[11]
W. B. Cairncross, D. N. Gresh, M. Grau, K. C. Cossel, T. S. Roussy, Y. Ni, Y. Zhou, J. Ye, and E. A. Cornell, Phys. Rev. Lett.119, 153001 (2017)
work page 2017
- [12]
- [13]
-
[14]
T. P. Harty, D. T. C. Allcock, C. J. Ballance, L. Guidoni, H. A. Janacek, N. M. Linke, D. N. Stacey, and D. M. Lucas, Phys. Rev. Lett.113, 220501 (2014)
work page 2014
-
[15]
P. Wang, C.-Y. Luan, M. Qiao, M. Um, J. Zhang, Y. Wang, X. Yuan, M. Gu, J. Zhang, and K. Kim, Nature Communi- cations12, 233 (2021)
work page 2021
-
[16]
C. J. Ballance, T. P. Harty, N. M. Linke, M. A. Sepiol, and D. M. Lucas, Phys. Rev. Lett.117, 060504 (2016)
work page 2016
-
[17]
R. Srinivas, S. C. Burd, H. M. Knaack, R. T. Sutherland, A. Kwiatkowski, S. Glancy, E. Knill, D. J. Wineland, D. Leibfried, A. C. Wilson, D. T. C. Allcock, and D. H. Slichter, Nature597, 209 (2021)
work page 2021
-
[18]
C. Ryan-Anderson, N. C. Brown, C. H. Baldwin, J. M. Dreiling, C. Foltz, J. P. Gaebler, T. M. Gatterman, N. Hewitt, C. Holliman, C. V. Horst, J. Johansen, D. Lucchetti, T. Mengle, M. Matheny, Y. Matsuoka, K. Mayer, M. Mills, S. A. Moses, B. Neyenhuis, J. Pino, P. Siegfried, R. P. Stutz, J. Walker, and D. Hayes, “High-fidelity and Fault-tolerant Teleportati...
-
[19]
S. A. Moses, C. H. Baldwin, M. S. Allman, R. Ancona, L. Ascarrunz, C. Barnes, J. Bartolotta, B. Bjork, P. Blanchard, M. Bohn, J. G. Bohnet, N. C. Brown, N. Q. Burdick, W. C. Burton, S. L. Campbell, J. P. Campora, C. Carron, J. Chambers, J. W. Chan, Y. H. Chen, A. Chernoguzov, E. Chertkov, J. Colina, J. P. Curtis, R. Daniel, M. DeCross, D. Deen, C. Delaney...
work page 2023
-
[20]
A. D. Leu, M. F. Gely, M. A. Weber, M. C. Smith, D. P. Nadlinger, and D. M. Lucas, Phys. Rev. Lett.131, 120601 (2023)
work page 2023
-
[21]
Z. Cai, C. Y. Luan, L. Ou, H. Tu, Z. Yin, J. N. Zhang, and K. Kim, J. Korean Phys. Soc.82, 882 (2023)
work page 2023
-
[22]
M. A. Weber, M. F. Gely, R. K. Hanley, T. P. Harty, A. D. Leu, C. M. L¨ oschnauer, D. P. Nadlinger, and D. M. Lucas, Phys. Rev. A110, L010601 (2024)
work page 2024
-
[23]
K. Wright, K. M. Beck, S. Debnath, J. M. Amini, Y. Nam, N. Grzesiak, J.-S. Chen, N. C. Pisenti, M. Chmielewski, C. Collins, K. M. Hudek, J. Mizrahi, J. D. Wong-Campos, S. Allen, J. Apisdorf, P. Solomon, M. Williams, A. M. Ducore, A. Blinov, S. M. Kreikemeier, V. Chaplin, M. Keesan, C. Monroe, and J. Kim, Nat Commun10, 5464 (2019)
work page 2019
-
[24]
S. Debnath, N. M. Linke, C. Figgatt, K. A. Landsman, K. Wright, and C. Monroe, Nature536, 63 (2016)
work page 2016
-
[25]
C. Figgatt, A. Ostrander, N. M. Linke, K. A. Landsman, D. Zhu, D. Maslov, and C. Monroe, Nature572, 368 (2019). 19
work page 2019
- [26]
-
[27]
N. Grzesiak, R. Bl¨ umel, K. Wright, K. M. Beck, N. C. Pisenti, M. Li, V. Chaplin, J. M. Amini, S. Debnath, J.-S. Chen, and Y. Nam, Nat Commun11, 2963 (2020)
work page 2020
-
[28]
J.-S. Chen, E. Nielsen, M. Ebert, V. Inlek, K. Wright, V. Chaplin, A. Maksymov, E. P´ aez, A. Poudel, P. Maunz, and J. Gamble, Quantum8, 1516 (2024)
work page 2024
- [29]
-
[30]
Y. Wan, D. Kienzler, S. D. Erickson, K. H. Mayer, T. R. Tan, J. J. Wu, H. M. Vasconcelos, S. Glancy, E. Knill, D. J. Wineland, A. C. Wilson, and D. Leibfried, Science364, 875 (2019)
work page 2019
-
[31]
V. Kaushal, B. Lekitsch, A. Stahl, J. Hilder, D. Pijn, C. Schmiegelow, A. Bermudez, M. M¨ uller, F. Schmidt-Kaler, and U. Poschinger, AVS Quantum Science2, 014101 (2020)
work page 2020
-
[32]
J. M. Pino, J. M. Dreiling, C. Figgatt, J. P. Gaebler, S. A. Moses, M. S. Allman, C. H. Baldwin, M. Foss-Feig, D. Hayes, K. Mayer, C. Ryan-Anderson, and B. Neyenhuis, Nature592, 209 (2021)
work page 2021
-
[33]
C. Mordini, A. Ricci Vasquez, Y. Motohashi, M. M¨ uller, M. Malinowski, C. Zhang, K. K. Mehta, D. Kienzler, and J. P. Home, Phys. Rev. X15, 011040 (2025)
work page 2025
- [34]
- [35]
-
[36]
D. Leibfried, R. Blatt, C. Monroe, and D. Wineland, Reviews of Modern Physics75, 281 (2003)
work page 2003
- [37]
-
[38]
S.-T. Wang, C. Shen, and L.-M. Duan, Sci Rep5, 8555 (2015)
work page 2015
-
[39]
A. Bermudez, X. Xu, R. Nigmatullin, J. O’Gorman, V. Negnevitsky, P. Schindler, T. Monz, U. G. Poschinger, C. Hempel, J. Home, F. Schmidt-Kaler, M. Biercuk, R. Blatt, S. Benjamin, and M. M¨ uller, Physical Review X7, 041061 (2017)
work page 2017
- [40]
-
[41]
A. K. Ratcliffe, L. M. Oberg, and J. J. Hope, Physical Review A101, 052332 (2020)
work page 2020
-
[42]
M. J. Madsen, D. L. Moehring, P. Maunz, R. N. Kohn, L.-M. Duan, and C. Monroe, Phys. Rev. Lett.97, 040505 (2006)
work page 2006
-
[43]
W. C. Campbell, J. Mizrahi, Q. Quraishi, C. Senko, D. Hayes, D. Hucul, D. N. Matsukevich, P. Maunz, and C. Monroe, Phys. Rev. Lett.105, 090502 (2010)
work page 2010
-
[44]
J. Mizrahi, C. Senko, B. Neyenhuis, K. G. Johnson, W. C. Campbell, C. W. S. Conover, and C. Monroe, Phys. Rev. Lett. 110, 203001 (2013)
work page 2013
-
[45]
J. Mizrahi, B. Neyenhuis, K. G. Johnson, W. C. Campbell, C. Senko, D. Hayes, and C. Monroe, Applied Physics B114, 45 (2014)
work page 2014
-
[46]
V. M. Sch¨ afer, C. J. Ballance, K. Thirumalai, L. J. Stephenson, T. G. Ballance, A. M. Steane, and D. M. Lucas, Nature 555, 75 (2018)
work page 2018
-
[47]
J. D. Wong-Campos, S. A. Moses, K. G. Johnson, and C. Monroe, Physical Review Letters119, 230501 (2017)
work page 2017
-
[48]
J. J. Garc´ ıa-Ripoll, P. Zoller, and J. I. Cirac, Physical Review Letters91, 157901 (2003)
work page 2003
-
[49]
J. J. Garc´ ıa-Ripoll, P. Zoller, and J. I. Cirac, Physical Review A71, 062309 (2005)
work page 2005
-
[50]
S.-L. Zhu, C. Monroe, and L.-M. Duan, Physical Review Letters97, 050505 (2006)
work page 2006
-
[51]
Fast gates for ion traps by splitting laser pulses
CDB. Bentley, ARR. Carvalho, D. Kielpinski, and Hope, JJ, New Journal of Physics15, 043006 (2013), arXiv:1211.7156 [quant-ph]
work page internal anchor Pith review Pith/arXiv arXiv 2013
-
[52]
R. L. Taylor, C. D. B. Bentley, J. S. Pedernales, L. Lamata, E. Solano, A. R. R. Carvalho, and J. J. Hope, Scientific Reports7, 46197 (2017)
work page 2017
-
[53]
E. P. G. Gale, Z. Mehdi, L. M. Oberg, A. K. Ratcliffe, S. A. Haine, and J. J. Hope, Physical Review A101, 052328 (2020)
work page 2020
-
[54]
I. Savill-Brown, J. J. Hope, A. K. Ratcliffe, V. D. Vaidya, H. Liu, S. A. Haine, C. R. Viteri, and Z. Mehdi, “High-speed and high-connectivity two-qubit gates in long chains of trapped ions,” (2025), arXiv:2506.11385 [quant-ph]
- [55]
-
[56]
I. Savill-Brown, Z. Mehdi, A. K. Ratcliffe, V. D. Vaidya, H. Liu, S. A. Haine, C. R. Viteri, and J. J. Hope, “Error-Resilient Fast Entangling Gates for Scalable Ion-Trap Quantum Processors,” (2025), arXiv:2508.07593 [quant-ph]
-
[57]
Fast mixed-species quantum logic gates for trapped-ion quantum networks,
Z. Mehdi, V. D. Vaidya, I. Savill-Brown, P. Grosser, A. K. Ratcliffe, H. Liu, S. A. Haine, J. J. Hope, and C. R. Viteri, “Fast mixed-species quantum logic gates for trapped-ion quantum networks,” (2025), arXiv:2412.07185 [quant-ph]
-
[58]
A. K. Ratcliffe, R. L. Taylor, J. J. Hope, and A. R. R. Carvalho, Physical Review Letters120, 220501 (2018)
work page 2018
-
[59]
Mehdi, AK Ratcliffe, and JJ Hope, Phys
Z. Mehdi, AK Ratcliffe, and JJ Hope, Phys. Rev. A102, 012618 (2020)
work page 2020
- [60]
-
[61]
J.-Y. Ji, J. K. Kim, and S. P. Kim, Phys. Rev. A51, 4268 (1995)
work page 1995
-
[62]
This definition of the secular frequency is subtly different from the definition in terms of the Wronskian identityu∗ α(t) ˙uα(t)− uα(t) ˙u∗ α(t) = 2iωα [34]
- [63]
-
[64]
C. D. B. Bentley, A. R. R. Carvalho, and J. J. Hope, New Journal of Physics17, 103025 (2015)
work page 2015
-
[65]
D. J. Berkeland, J. D. Miller, J. C. Bergquist, W. M. Itano, and D. J. Wineland, Journal of Applied Physics83, 5025 (1998), https://pubs.aip.org/aip/jap/article-pdf/83/10/5025/18699946/5025\ 1\ online.pdf
work page 1998
-
[66]
A. Sørensen and K. Mølmer, Physical Review A62(2000), 10.1103/physreva.62.022311
- [67]
-
[68]
C. D. B. Bentley, R. L. Taylor, A. R. R. Carvalho, and J. J. Hope, Physical Review A93, 042342 (2016). 20
work page 2016
-
[69]
M. I. Hussain, M. J. Petrasiunas, C. D. B. Bentley, R. L. Taylor, A. R. R. Carvalho, J. J. Hope, E. W. Streed, M. Lobino, and D. Kielpinski, Opt. Express24, 16638 (2016)
work page 2016
-
[70]
D. Heinrich, M. Guggemos, M. Guevara-Bertsch, M. I. Hussain, C. F. Roos, and R. Blatt, New Journal of Physics21, 073017 (2019)
work page 2019
-
[71]
K. Shimizu, J. Scarabel, E. Bridge, S. Connell, M. Ghadimi, B. Haylock, M. I. Hussain, E. Streed, and M. Lobino, Applied Physics Letters119, 214003 (2021)
work page 2021
-
[72]
M. I. Hussain, M. Guevara-Bertsch, E. Torrontegui, J. J. Garcıa-Ripoll, R. Blatt, and C. F. Roos, arXiv [quant-ph] (2023)
work page 2023
-
[73]
K. G. Johnson, J. D. Wong-Campos, B. Neyenhuis, J. Mizrahi, and C. Monroe, Nature Communications8(2017), 10.1038/s41467-017-00682-6
-
[74]
K. G. Johnson, B. Neyenhuis, J. Mizrahi, J. D. Wong-Campos, and C. Monroe, Phys. Rev. Lett.115, 213001 (2015)
work page 2015
-
[75]
W.-X. Guo, Y.-K. Wu, Y.-Y. Huang, L. Feng, C.-X. Huang, H.-X. Yang, J.-Y. Ma, L. Yao, Z.-C. Zhou, and L.-M. Duan, Physical Review A106(2022), 10.1103/physreva.106.022608
-
[76]
H.-N. Wu, C. Zhang, J. Song, Y. Xia, and Z.-C. Shi, Phys. Rev. A107, 023103 (2023)
work page 2023
-
[77]
N. V. Vitanov, A. A. Rangelov, B. W. Shore, and K. Bergmann, Rev. Mod. Phys.89, 015006 (2017)
work page 2017
-
[78]
M. R. Dietrich, A. Avril, R. Bowler, N. Kurz, J. S. Salacka, G. Shu, B. B. Blinov, J. R. Danielson, and T. S. Pedersen, inAIP Conference Proceedings(AIP, New York (New York), 2009) pp. 25–30
work page 2009
-
[79]
I. D. Moore, W. C. Campbell, E. R. Hudson, M. J. Boguslawski, D. J. Wineland, and D. T. C. Allcock, Phys. Rev. A 107, 032413 (2023)
work page 2023
-
[80]
High-fidelity heralded quantum state preparation and measurement,
A. S. Sotirova, J. D. Leppard, A. Vazquez-Brennan, S. M. Decoppet, F. Pokorny, M. Malinowski, and C. J. Ballance, “High-fidelity heralded quantum state preparation and measurement,” (2024)
work page 2024
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.