Multi-stage Stern-Gerlach experiment modeled (with additional appendices)
Pith reviewed 2026-05-24 11:55 UTC · model grok-4.3
The pith
The physical co-quantum concept accounts for multi-stage Stern-Gerlach observations by predicting beam fractions in absolute units with no parameter adjustment.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Introducing the physical co-quantum concept provides a plausible physical mechanism for the multi-stage Stern-Gerlach experiment and predicts the experimental observation in absolute units without fitting with a p-value less than one per million. The co-quantum concept is corroborated by statistically reproducing exactly the wave function, density operator, and uncertainty relation for electron spin.
What carries the argument
The physical co-quantum concept, an independent physical entity applied to the Stern-Gerlach apparatus to generate the observed beam fractions.
If this is right
- The Majorana and Rabi formulae diverge from the data while the co-quantum approach matches it exactly.
- The match is obtained in absolute units with no parameters adjusted.
- The wave function, density operator, and uncertainty relation for electron spin are reproduced by the same rules.
- The p-value below one per million indicates the match is unlikely to occur by chance alone.
Where Pith is reading between the lines
- The co-quantum rules might underlie the emergence of standard quantum features in sequential spin measurements.
- The same concept could be checked for consistency in other atomic or quantum-optics setups that involve staged spin projections.
- If the concept holds, it would supply a concrete physical account of spin-state reduction that standard postulates leave unspecified.
Load-bearing premise
The physical co-quantum concept is a valid independent physical entity whose rules can be applied to the Stern-Gerlach apparatus to generate the observed beam fractions without dependence on the target data.
What would settle it
A repetition of the multi-stage Stern-Gerlach experiment that produces beam fractions differing substantially from the absolute predictions of the co-quantum model.
read the original abstract
In the classic multi-stage Stern$-$Gerlach experiment conducted by Frisch and Segr\`e, the Majorana (Landau$-$Zener) and Rabi formulae diverge afar from the experimental observation while the physical mechanism for electron-spin collapse remains unidentified. Here, introducing the physical co-quantum concept provides a plausible physical mechanism and predicts the experimental observation in absolute units without fitting (i.e., no parameters adjusted) with a p-value less than one per million, which is the probability that the co-quantum theory happens to match the experimental observation purely by chance. Further, the co-quantum concept is corroborated by statistically reproducing exactly the wave function, density operator, and uncertainty relation for electron spin in Stern$-$Gerlach experiments.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript introduces a new 'physical co-quantum' concept as a mechanism for electron-spin collapse in the multi-stage Stern-Gerlach experiment of Frisch and Segrè. It asserts that this concept yields an exact, parameter-free prediction of the observed beam fractions (in absolute units), reports a p-value < 10^{-6} against chance agreement, and additionally reproduces the standard quantum-mechanical wave function, density operator, and uncertainty relation for spin.
Significance. If the co-quantum postulates can be shown to be fixed and independent of the target Frisch-Segrè fractions, the work would supply a concrete physical mechanism for spin measurement outcomes together with a falsifiable, zero-parameter prediction; such a result would be of clear interest to quantum foundations. The additional claim of exact reproduction of the standard spin formalism is a further point of potential strength if the mapping is derived rather than stipulated.
major comments (3)
- [Abstract / main text] Abstract and main text: the central claim of a parameter-free prediction requires the co-quantum interaction/collapse rules to be stated explicitly and prior to any application to the Frisch-Segrè data. No such postulates (interaction Hamiltonian, statistical mapping, or collapse criterion) appear in the provided text, so the 'no parameters adjusted' assertion and the reported p-value cannot be verified.
- [Abstract] Abstract: the p-value < 10^{-6} is asserted without any description of the underlying statistical model, the null hypothesis, the number of independent trials, or the method used to compute the probability that the co-quantum theory matches the data by chance.
- [Main text] Main text (co-quantum definition): the physical co-quantum is introduced with the sole stated justification that it reproduces the target experimental fractions and the standard quantum spin formalism. This structure is consistent with a definition chosen to match the data rather than an independent derivation, directly undermining the 'parameter-free' and 'p-value' claims.
minor comments (1)
- [Title / appendices] The manuscript title mentions 'additional appendices' but the provided text does not indicate whether the appendices contain the missing explicit postulates or the p-value derivation.
Simulated Author's Rebuttal
We thank the referee for the careful and constructive review. We agree that the co-quantum postulates must be stated explicitly and prior to the data application, and that the statistical details underlying the p-value claim require full specification. We will revise the manuscript to address these issues directly.
read point-by-point responses
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Referee: [Abstract / main text] Abstract and main text: the central claim of a parameter-free prediction requires the co-quantum interaction/collapse rules to be stated explicitly and prior to any application to the Frisch-Segrè data. No such postulates (interaction Hamiltonian, statistical mapping, or collapse criterion) appear in the provided text, so the 'no parameters adjusted' assertion and the reported p-value cannot be verified.
Authors: We accept this criticism. Although the manuscript introduces the co-quantum concept as the mechanism that yields the exact, parameter-free match, the explicit interaction and collapse rules are not isolated and presented before the Frisch-Segrè analysis. In the revised version we will insert a dedicated subsection that enumerates the postulates (interaction rules, statistical mapping, and collapse criterion) at the outset of the main text, prior to any comparison with experiment. This will make the parameter-free character verifiable. revision: yes
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Referee: [Abstract] Abstract: the p-value < 10^{-6} is asserted without any description of the underlying statistical model, the null hypothesis, the number of independent trials, or the method used to compute the probability that the co-quantum theory matches the data by chance.
Authors: We agree that the statistical procedure is not described. The revised manuscript will contain an explicit account of the statistical model, the null hypothesis (random agreement with the observed beam fractions), the number of independent trials or measurements, and the precise method by which the probability p < 10^{-6} is obtained. This material will be placed in a new appendix so that the p-value claim can be independently checked. revision: yes
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Referee: [Main text] Main text (co-quantum definition): the physical co-quantum is introduced with the sole stated justification that it reproduces the target experimental fractions and the standard quantum spin formalism. This structure is consistent with a definition chosen to match the data rather than an independent derivation, directly undermining the 'parameter-free' and 'p-value' claims.
Authors: The co-quantum rules are fixed once and for all by the requirement that they furnish a physical mechanism for spin collapse; the same fixed rules then produce both the Frisch-Segrè fractions without adjustment and the standard spin formalism. Nevertheless, the present ordering may give the impression of a data-driven definition. We will therefore restructure the main text so that the postulates appear first as an independent proposal, followed by their application to the experiment and only then by the demonstration that they recover the quantum-mechanical results. This reordering will clarify that the rules are not chosen after the fact to fit the data. revision: partial
Circularity Check
No significant circularity identified from provided text
full rationale
The abstract asserts that the co-quantum concept predicts the Frisch-Segrè fractions in absolute units with no parameters adjusted. No equations, definitions, or derivation steps are supplied in the visible text that would allow verification of self-definition, fitted inputs renamed as predictions, or load-bearing self-citations. The claim of independence is stated explicitly, and the paper positions the concept as supplying a prior physical mechanism rather than a post-hoc fit. Absent any quoted reduction showing the target data entering the postulates by construction, the derivation chain cannot be shown to collapse to its inputs.
Axiom & Free-Parameter Ledger
axioms (1)
- ad hoc to paper The physical co-quantum concept exists and supplies the mechanism for electron-spin collapse in Stern-Gerlach experiments.
invented entities (1)
-
physical co-quantum
no independent evidence
Reference graph
Works this paper leans on
-
[1]
Zeitschrift f¨ ur Physik9(1), 349–352 (1922)
Gerlach W, Stern O. Der experimentelle nachweis der richtungsquantelung im magnetfeld. Zeitschrift für Physik. 1922;9(1):349-52. doi: 10.1007/BF01326983
-
[2]
The Stern - Gerlach experiment revisited
Schmidt-Böcking H, Schmidt L, Lüdde HJ, Trageser W, Templeton A, Sa uer T. The Stern - Gerlach experiment revisited. The European Physical Journal H. 2016;41(4):327- 64. doi: 10.1140/epjh/e2016-70053-2
-
[3]
The Stern –Gerlach experiment at 100
Castelvecchi D. The Stern –Gerlach experiment at 100. Nature Reviews Physics. 2022. doi: 10.1038/s42254-022-00436-4
-
[4]
Quantentheoretische bemerkungen zum experiment von Stern und Gerlach
Ei nstein A, Ehrenfest P. Quantentheoretische bemerkungen zum experiment von Stern und Gerlach. Zeitschrift für Physik. 1922;11(1):31-4. doi: 10.1007/BF01328398
-
[5]
The Stern–Gerlach experiment and the effects of spin relaxation
Wennerström H, Westlund P-O. The Stern–Gerlach experiment and the effects of spin relaxation. Physical Chemistry Chemical Physics. 2012;14(5):1677-84. doi: 10.1039/C2CP22173J
-
[6]
The pilot-wave perspective on spin
Norsen T. The pilot-wave perspective on spin. Am J Phys. 2014;82(4):337-48
work page 2014
-
[7]
The Feynman Lectures on Physics
Feynman RP, Leighton RB, Sands ML. The Feynman Lectures on Physics. Reading, Mass.: Addison-Wesley Pub. Co.; 1963
work page 1963
-
[8]
Über die einstellung der richtungsquantelung
Phipps TE, Stern O. Über die einstellung der richtungsquantelung. Zeitschrift für Physik. 1932;73(3):185-91. doi: 10.1007/BF01351212
-
[9]
Über die einstellung der richtungsquantelung
Frisch R, Segrè E. Über die einstellung der richtungsquantelung. II. Zeitschrift für Physik. 1933;80(9):610-6. doi: 10.1007/BF01335699
-
[10]
Atomi orientati in campo magnetico variabile
Majorana E. Atomi orientati in campo magnetico variabile. Il Nuovo Cimento (1924- 1942). 1932;9(2):43-50. doi: 10.1007/BF02960953
-
[11]
Oriented atoms in a variable magnetic field
Majorana E. Oriented atoms in a variable magnetic field. In: Bassani G, editor. Ettore Majorana: Scientific Papers. Bologna, Berlin: Società Italian die Fisica and Springer; 2006. p. 125-32
work page 2006
-
[12]
Zur theorie der energieubertragung
Landau L. Zur theorie der energieubertragung. II. Physikalische Zeitschrift der Sowjetunion. 1932;2:46–51
work page 1932
-
[13]
Non-adiabatic crossing of energy levels
Zener C. Non-adiabatic crossing of energy levels. Proceedings of the Royal Society of London Series A. 1932;137:696
work page 1932
-
[14]
Theorie der unelastischen Stösse zwischen atomen
Stueckelberg ECG. Theorie der unelastischen Stösse zwischen atomen. Helvetica Physica Acta. 1932;5:369
work page 1932
-
[15]
Nonadiabatic Landau–Zener–Stückelberg–Majorana transitions, dynamics, and interference
Ivakhnenko OV, Shevchenko SN, Nori F. Nonadiabatic Landau–Zener–Stückelberg–Majorana transitions, dynamics, and interference. Physics Reports. 2023;995:1- 89. doi: 10.1016/j.physrep.2022.10.002
-
[16]
On the process of space quantization
Rabi II. On the process of space quantization. Physical Review. 1936;49(4):324- 8. doi: 10.1103/PhysRev.49.324
-
[17]
Derivation from Bloch Equation to von Neumann Equation to Schrödinger –Pauli Equation
Wang LV. Derivation from Bloch Equation to von Neumann Equation to Schrödinger –Pauli Equation. Found Phys. 2022;52(3):61
work page 2022
-
[18]
Present status and future challenges of non- interferometric tests of collapse models
Carlesso M, Donadi S, Ferialdi L, Paternostro M, Ulbricht H, Bassi A. Present status and future challenges of non- interferometric tests of collapse models. Nature Physics. 2022. doi: 10.1038/s41567-021-01489-5
-
[19]
Unified dynamics for microscopic and macroscopic systems
Ghirardi GC, Rimini A, Weber T. Unified dynamics for microscopic and macroscopic systems. Phys Rev D. 1986;34(2):470-91. doi: 10.1103/physrevd.34.470
-
[20]
Combining stochastic dynamical state-vector reduction with spontaneous localization
Pearle P. Combining stochastic dynamical state-vector reduction with spontaneous localization. Physical Review A. 1989;39(5):2277
work page 1989
-
[21]
Ghirardi GC, Pearle P, Rimini A. Markov processes in Hilbert space and continuous spontaneous localization of systems of identical particles. Physical Review A. 1990;42(1):78- 89. doi: 10.1103/physreva.42.78. 19
-
[22]
Principles and Procedures of Statistics
Steel RGD, Torrie JH. Principles and Procedures of Statistics. New York: McGraw Hill; 1960
work page 1960
-
[23]
A Course in Theoretical Statistics
Rahman N. A Course in Theoretical Statistics. New York: Charles Griffin and Company; 1968
work page 1968
-
[24]
The Jeffreys –Lindley paradox and discovery criteria in high energy physics
Cousins RD. The Jeffreys –Lindley paradox and discovery criteria in high energy physics. Synthese. 2017;194(2):395-432
work page 2017
-
[25]
doi:10.1103/PhysRevLett.116.061102 , keywords =
Abbott BP, Abbott R, Abbott TD, Abernathy MR, Acernese F, Ackley K, et al. Observation of Gravitation al Waves from a Binary Black Hole Merger. Phys Rev Lett. 2016;116(6). doi: 10.1103/physrevlett.116.061102
-
[26]
Introduction to Quantum Optics: from the Semi -classical Approach to Quantized Light
Grynberg G, Aspect A, Fabre C. Introduction to Quantum Optics: from the Semi -classical Approach to Quantized Light. Cambridge University Press; 2010
work page 2010
-
[27]
Geometrical representation of the Schrödinger equation for solving maser problems
Feynman RP, Vernon Jr FL, Hellwarth RW. Geometrical representation of the Schrödinger equation for solving maser problems. Journal of applied physics. 1957;28(1):49-52
work page 1957
-
[28]
A phenomenological theory of damping in ferromagnetic materia ls
Gilbert TL. A phenomenological theory of damping in ferromagnetic materia ls. IEEE Transactions on Magnetics. 2004;40(6):3443-9. doi: 10.1109/TMAG.2004.836740
-
[29]
https://periodic.lanl.gov/19.shtml Accessed
Los Alamos National Laboratory: Periodic Table of Elements. https://periodic.lanl.gov/19.shtml Accessed
-
[30]
Foundations of Quantum Mechanics
Norsen T. Foundations of Quantum Mechanics. Springer; 2017
work page 2017
-
[31]
Introduction to Electrodynamics
Griffiths DJ. Introduction to Electrodynamics. 4th ed. Cambridge University Press; 2017
work page 2017
-
[32]
Jackson JD. Classical Electrodynamics. USA: John Wiley & Sons; 1999
work page 1999
-
[33]
Ohanian HC. What is spin? Am J Phys. 1986;54(6):500-5. doi: 10.1119/1.14580
-
[34]
Use of rotating coordinates in magnetic resonance problems
Rabi II, Ramsey NF, Schwinger J. Use of rotating coordinates in magnetic resonance problems. Reviews of Modern Physics. 1954;26(2):167
work page 1954
-
[35]
Forbes MD, Jarocha LE, Sim S, Tarasov VF. Time-resolved electron paramagnetic resonance spectroscopy: History, technique, and application to supramolecular and macromolecular chemistry. In: Williams IH, Williams NH, editors. Advances in Physical Organic Chemistry. Elsevier; 2013. p. 1-83
work page 2013
-
[36]
Gas Phase NMR for the Study of Chemical Reactions: Kinetics and Product Identification
Marchione AA, Conklin B. Gas Phase NMR for the Study of Chemical Reactions: Kinetics and Product Identification. In: Jackowski K, Jaszuński M, editors. Gas Phase NMR. Cambridge: Royal Society of Chemistry; 2016. p. 126-51
work page 2016
-
[37]
A s pin flipper for reversal of polarisation in a thermal atomic beam
Schroder W, Baum G. A s pin flipper for reversal of polarisation in a thermal atomic beam. Journal of Physics E: Scientific Instruments. 1983;16(1):52
work page 1983
-
[38]
Breit G, Rabi I. Measurement of nuclear spin. Physical Review. 1931;38(11):2082
work page 1931
-
[39]
Barra AL, Hassan AK. Electron Spin Re sonance. In: Bassani F, Liedl GL, Wyder P, editors. Encyclopedia of Condensed Matter Physics. Oxford: Elsevier; 2005. p. 58-67
work page 2005
-
[40]
Is Quantum Theory Exact? Science
Adler SL, Bassi A. Is Quantum Theory Exact? Science. 2009;325(5938):275- 6. doi: doi:10.1126/science.1176858
-
[41]
Making Sense of Quantum Mechanics
Bricmont J. Making Sense of Quantum Mechanics. Springer; 2016
work page 2016
-
[42]
Do We Really Understand Quantum Mechanics? Cambridge University Press; 2019
Laloë F. Do We Really Understand Quantum Mechanics? Cambridge University Press; 2019
work page 2019
-
[43]
The Quantum Mechanics Conundrum: Interpretation and Foundations
Auletta G. The Quantum Mechanics Conundrum: Interpretation and Foundations. Springer; 2019
work page 2019
-
[44]
Can quantum-mechanical description of physical reality be considered complete
Einstein A, Podolsky B, Rosen N. Can quantum-mechanical description of physical reality be considered complete. Physical Review. 1935;47(10):777-80. doi: 10.1103/PhysRev.47.777
-
[45]
Quantum theory cannot consistently describe the use of itself
Frauchiger D, Renner R. Quantum theory cannot consistently describe the use of itself. Nature Communications. 2018;9(1):3711. doi: 10.1038/s41467-018-05739-8
-
[46]
Die gegenwärtige situation in der quantenmechanik
Schrödinger E. Die gegenwärtige situation in der quantenmechanik. Naturwissenschaften. 1935;23:807. 20
work page 1935
-
[47]
Titimbo K, Garrett DC, Kahraman SS, He Z, Wang LV. Numerical m odeling of the multi - stage Stern-Gerlach experiment by Frisch and Segre using co- quantum dynamics via the Bloch equation. arXiv preprint arXiv:220813444. 2022
work page 2022
-
[48]
He Z, Titimbo K, Garrett DC, Kahraman SS, Wang LV. Numerical modeling of the multi - stage St ern-Gerlach experiment by Frisch and Segre using co -quantum dynamics via the Schrodinger equation. arXiv preprint arXiv:220814588. 2022
work page 2022
-
[49]
Bloch F. Nuclear Induction. Physical Review. 1946;70(7- 8):460-74. doi: 10.1103/physrev.70.460
-
[50]
Kahraman SS, Titimbo K, He Z, Shen J -T, Wang LV. Quantum mechanical modeling of the multi-stage Stern-Gerlach experiment by Frisch and Segre using the von Neumann equation. arXiv preprint arXiv:221011553. 2022
work page 2022
-
[51]
Double Stern- Gerlach experiments o n Mn@ Sn 12: Refocusing of a paramagnetic superatom
Fuchs TM, Schäfer R. Double Stern- Gerlach experiments o n Mn@ Sn 12: Refocusing of a paramagnetic superatom. Physical Review A. 2018;98(6):063411
work page 2018
-
[52]
Remarks concerning the essays brought together in this co- operative volume
Einstein A. Remarks concerning the essays brought together in this co- operative volume. In: Schilpp PA, editor. Albert Einstein: Philosopher -Scientist. Library of Living Philosophers. La Salle: Open Court; 1949. p. 665-88
work page 1949
-
[53]
Relativistic Quantum Mechanics
Bjorken JD, Drell SD. Relativistic Quantum Mechanics. New York: Mcgraw -Hill College; 1964
work page 1964
-
[54]
The magnetic moment of the K 39 nucleus
Gibbons JJ, Bartlett JH. The magnetic moment of the K 39 nucleus. Physical Review. 1935;47(9):692-4. doi: 10.1103/physrev.47.692
-
[55]
Results of calculations of atomic wave functions
Hartree DR. Results of calculations of atomic wave functions. II.—Results for K + and Cs+. Proceedings of the Royal Society of London Series A. 1934;143(850):506-17
work page 1934
-
[56]
Wittig C. The Landau−Zener formula. J Phys Chem B. 2005;109(17):8428- 30. doi: 10.1021/jp040627u
-
[57]
Majorana and condensed matter physics
Wilczek F. Majorana and condensed matter physics. In: Esposito S, editor. The Physics of Ettore Majorana: Theoretical, Mathematical, and Phenomenological. Cambridge University Press
-
[58]
Majorana's approach to nonadiabatic transitions validates the adiabatic-impulse approximation
Kofman PO, Ivakhnenko OV, Shevchenko SN, Nori F. Majorana's approach to nonadiabatic transitions validates the adiabatic-impulse approximation. arXiv preprint arXiv:220800481. 2022
work page 2022
-
[59]
Fundamentals of Quantum Optics and Quantum Information
Lambropoulos P, Petrosyan D. Fundamentals of Quantum Optics and Quantum Information. Springer; 2007
work page 2007
-
[60]
On the problem of hidden variables in quantum mechanics
Bell JS. On the problem of hidden variables in quantum mechanics. Reviews of Modern Physics. 1966;38(3):447-52. doi: 10.1103/RevModPhys.38.447
-
[61]
Bell correlations between spatially separated pairs of atoms
Shin DK, Henson BM, Hodgman SS, Wasak T, Chwedeńczuk J, Truscott AG. Bell correlations between spatially separated pairs of atoms. Nature Communications. 2019;10(1). doi: 10.1038/s41467-019-12192-8
-
[62]
A matter wave Rarity -Tapster interferometer to demonstrate non -locality
Thomas KF, Henson BM, Wang Y, Lewis-Swan RJ, Kheruntsyan KV, Hodgman SS, et al. A matter wave Rarity -Tapster interferometer to demonstrate non -locality. arXiv preprint arXiv:220608560. 2022
work page 2022
-
[64]
Coincidentally, this solution differs from the Gaussian solution (Eq
based on Hartree’s self-consistent field [55], we numerically reached 𝐵𝐵�⃗𝑛𝑛= 0.138𝜇𝜇0 𝜋𝜋𝑅𝑅3 𝜇𝜇⃗𝑛𝑛, (51) where the average radius is set to 𝑅𝑅. Coincidentally, this solution differs from the Gaussian solution (Eq. 50) by only 2%. Table S1. Normalized 𝑃𝑃(4𝑠𝑠) for potassium. 𝜓𝜓𝑟𝑟(0) = � 9.76 (4𝜋𝜋)⁄ and 𝜓𝜓𝑟𝑟(𝑟𝑟) = 𝑃𝑃� � 4𝜋𝜋𝑎𝑎0𝑟𝑟�⁄ for 𝑟𝑟> 0. [54] 𝒓𝒓𝒂𝒂𝟎𝟎⁄ 𝑷𝑷 ...
work page 1967
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[65]
up” for magnetic moment and hence “down
(94) 33 Here, 𝐼𝐼 denotes the current carried by the wire along the −𝑥𝑥 axis, and 𝐵𝐵𝑟𝑟 (0.42 × 10−4 T) denotes the uniformly distributed remnant (residual) fringe magnetic flux density , which is parallel with the +𝑧𝑧 axis. The magnetic field generated by the wire cancels the remnant field at the null point (NP) to produce a n approximate quadrupole (Fig. ...
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[66]
(179) The even split between the two ±𝑥𝑥 branches is because the heart shape associated with either of the ±𝑧𝑧 branches is rotationally symmetric about the 𝑧𝑧 axis. Thus, the wave function is |𝜇𝜇̂𝑒𝑒⟩𝑥𝑥= 1 √2 |+𝑥𝑥⟩ + 1 √2 exp(𝑖𝑖𝜙𝜙𝑒𝑒𝑥𝑥) |−𝑥𝑥⟩. (180) We derive the standard deviation, Δ𝑠𝑠𝑥𝑥, as follows: 〈𝑠𝑠𝑥𝑥〉 = − ℏ 2 � 1 √2� 2 + ℏ 2 � 1 √2� 2 = 0, (181) 〈𝑠𝑠𝑥...
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