REVIEW 3 major objections 5 minor 4 cited by
High-Density Ultracold Neutron Source for Low-Energy Particle Physics Experiments
T0 review · 3 major / 5 minor · reviewed 2026-08-16 · deepseek-v4-flash
Pith's one-line read SuperSUN, a superfluid-helium converter, reports a record stored ultracold-neutron density of 273 per cubic centimeter and 60 days of continuous operation.
desk verdict A real experimental milestone with internally consistent numbers—record stored UCN density is a lower bound, but the 'highest ever measured' claim needs a quantitative comparison baseline. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The mechanism is superthermal UCN production: a cold neutron with wavelength $0.89\,\mathrm{nm}$ scatters in superfluid helium-4 and creates a single phonon, transferring nearly all its energy and momentum, so the neutron becomes ultracold. In isotopically pure helium-4 there is no neutron absorption, and upscattering out of the UCN energy range is negligible below about 0.6 K, so losses can approach the neutron $\beta$-decay limit. The apparatus multiplies production by guiding the cold beam through a 3-meter-long supermirror-lined converter, uses a CYTOP fluoropolymer coating to reduce wall losses, and seals the extraction aperture with a movable diamond-like-carbon valve; stored UCN leave through coated guides and are counted by a helium-3 detector.
What would settle it
Measure the in-situ density by a method that does not rely on extracting neutrons through guides—for example, a small calibrated UCN detector inserted directly into the converter, or an independent measurement of production rate and total loss rate to predict saturation density. If such a measurement gives a value well below $273\,\mathrm{cm}^{-3}$ after accounting for extraction losses, the record-density claim would be overturned; conversely, an independent in-situ measurement near $273\,\mathrm{cm}^{-3}$ would confirm it.
Extended reading notes
Core claim
The central claim is that SuperSUN achieves the highest stored ultracold-neutron density ever measured: $273\,\mathrm{cm}^{-3}$ in-situ, obtained by accumulating for 1500 seconds with a closed valve and then extracting $3.88\times 10^6$ UCN into a detector, dividing by the 14.2-liter converter volume without corrections. The same source demonstrates continuous 'open converter' operation with a steady extraction rate of $2.1\times 10^4\,\mathrm{s}^{-1}$ sustained over a full 60-day reactor cycle. Storage and accumulation are characterized by bi-exponential time constants near 130 s and 410 s, and the paper shows that the stored spectrum becomes softer, and hence less lossy, with longer accumulation or holding time. The paper argues that soft spectra and long storage times make the source suited to storage experiments that hold neutrons for hundreds of seconds, not just to beam-flux measurements.
Load-bearing premise
The result assumes that the 3.88 million ultracold neutrons counted after extraction equal the number stored inside the 14.2-liter converter: no corrections are applied for detector efficiency, transport through guides and windows, the roughly 5% of neutrons too low in energy to leave the source, or pileup; if those combined corrections are large, the true in-situ density could differ from $273\,\mathrm{cm}^{-3}$.
Editorial extensions
If this is right
- A stored in-situ density of $273\,\mathrm{cm}^{-3}$, if taken at face value, makes SuperSUN the benchmark for future UCN storage experiments; no other source has demonstrated a higher density under this measurement convention.
- The measured accumulation and storage time constants (roughly 130 s and 410 s) imply that storage experiments can operate with repetition periods of a few minutes and still reach close to saturation density, the operating regime projected for a competitive neutron electric dipole moment search.
- Continuous 60-day operation shows the source can support full reactor cycles as a user facility, not just short proof-of-principle runs.
- The spectral softening with holding time provides a starting point for modeling energy-dependent losses in any experiment using this source.
Reading between the lines
- If the density claim survives a calibration of detector efficiency and transport losses, it would suggest that superfluid-helium superthermal converters can exceed the phase-space density of existing reactor- and spallation-based UCN sources for storage applications, which could change the economic case for building dedicated UCN facilities.
- The planned addition of a superconducting octupole magnet should allow a direct test of magnetic trapping inside the same converter: comparing saturated densities with the magnet on and off would isolate the gain from the magnetic reflector, a measurement this paper does not report.
- The observed degradation of about 3% per day in total UCN output without a separation foil implies that long-duration science runs will need the polypropylene foil; an A/B comparison of daily output with and without the foil would separate the foil's static 10% transmission loss from its protective benefit.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper reports the first measurements from SuperSUN, a new superthermal ultracold-neutron (UCN) source at the Institut Laue-Langevin that uses isotopically pure superfluid 4He below 0.6 K. The authors claim continuous operation over 60 days, a continuous UCN extraction rate of 2.1e4 s^-1, and a saturated stored UCN density of 273 cm^-3, obtained by dividing the 3.88e6 UCN detected after extraction by the 14.2-liter converter volume. They characterize UCN accumulation and storage with phenomenological multi-exponential fits, reporting time constants of about 131 s and 410 s for accumulation and 117 s and 414 s for storage. The paper argues that this is the highest stored UCN density ever measured and discusses implications for the PanEDM experiment and future in-situ storage experiments.
Significance. If the measurements are correct, this is a major advance for ultracold-neutron science: the highest stored UCN density reported to date, with a soft spectrum and long storage times, would enable qualitatively new precision experiments. The central arithmetic is internally consistent and reproducible: 3.88e6 / 14.2e3 cm^3 = 273 cm^-3. The measurements are direct, and the quoted density, being uncorrected for detection and extraction losses, is a conservative lower bound on the true in-situ density; this is a genuine strength. The paper also clearly labels its fitting functions as phenomenological, avoiding any over-interpretation of the time constants. The primary weakness is that the comparative claim 'highest ever measured' is not supported by a quantitative baseline against published UCN densities, and the abstract presents the density without the qualifiers that the body text uses.
major comments (3)
- [Summary and outlook; Abstract; Introduction] The claim that 273 cm^-3 is 'the highest ever measured' (or 'the largest UCN density stored and measured to date') is not substantiated by a quantitative comparison with previously reported UCN densities. The paper cites earlier sources [19,21,42-44] but does not give their densities or a table of values, and the factor-14 comparison in the Introduction refers to production rates, not stored density. Since this record claim is a central headline of the paper, please provide a quantitative comparison with published UCN densities, specifying the correction status and definition used for each, or temper the claim accordingly.
- [Characterization, paragraph 3; Abstract] The value 273 cm^-3 is labeled 'saturated in-situ density' in the abstract but is actually obtained by dividing the number of UCN detected after extraction (3.88e6) by the converter volume (14.2 L), with no corrections applied. As the text notes, this count excludes the ~5% of UCN unable to exit the source (footnote [39]), pileup losses of up to 10%, and unquantified detector and transport efficiencies; it is therefore a conservative lower bound on the true in-situ number density, not a direct in-situ measurement. Please state in the abstract and summary that this is an uncorrected lower bound derived from extracted counts, and where possible give an estimate of the total correction factor.
- [Abstract; Apparatus, paragraph 2] The abstract claims that 'continuous operation with an intense broad-spectrum cold neutron beam is demonstrated over 60 days,' but no data or run log supporting this 60-day period appears in the manuscript. The body text only states that the source 'operates continuously for full reactor cycles, typically 7-9 weeks,' with weekly reservoir refills. Since continuous operation over 60 days is one of the paper's stated firsts, please provide a supporting timeline, a statement of the actual achieved continuous run, or remove the specific '60 days' claim from the abstract.
minor comments (5)
- [Abstract] The abstract uses '21000 s^-1' whereas the text uses '2.1 × 10^4 s^-1'; please use one consistent notation throughout.
- [Introduction, paragraph 2] The phrase 'exceeding earlier demonstrations by a factor 14 [19,21]' refers to UCN production, not stored density; please clarify this in the text so it is not read as a density comparison.
- [Footnote [39]] The statement that ~5% of produced UCN cannot exit would be more useful if accompanied by the estimated energy threshold and the fraction of the spectrum below it, rather than only the percentage.
- [References [40]] Reference [40] for the DUNya-type detector is from 1974; please check that this is the appropriate primary reference, or add a more recent characterization reference.
- [Characterization, paragraph 1] The detected leakage rate of ~80 s^-1 through the monitoring hole during accumulation is a useful systematics check; please state whether this leakage is included in the total UCN production estimate or corrected for in the reported 3.88e6 extracted UCN.
Circularity Check
No significant circularity: the headline density is a direct ratio of counted UCN to converter volume, with caveats explicitly stated and no fitted parameter used as a prediction.
full rationale
The paper's central quantitative claims are direct measurements rather than derived outputs of a fit or of a self-citation chain. The stored density is computed as 3.88e6 detected UCN divided by the 14.2-liter converter volume, giving 273 cm^-3; this is simple arithmetic on independent inputs (detected counts and stated volume), and the paper explicitly calls it "uncorrected" and therefore a conservative lower bound, with the main caveats disclosed in footnote [39] and in the pileup discussion. The phenomenological time constants in Eqs. (1)-(5) are fitted to the data and are explicitly labeled "essentially phenomenological," so they are not dressed up as first-principles predictions. Self-citations such as Refs. [19,21,28,29] serve as prior prototype results, design-goal references, and context for comparison; they are not used to force the present density or rates by construction. The soft spot identified by the skeptic, namely the "highest ever measured" comparative claim lacking a quantitative table of prior source densities, is a verifiability or completeness issue, not circularity, because the present measurement does not depend on those prior values for its own validity. No step in the paper reduces to its own inputs by definition, so the appropriate circularity score is 0.
Assumptions & free parameters
free parameters (2)
- Storage extraction profile parameters (c, tau_3, tau_4) =
c = 0.17 +/- 0.02, tau_3 = 117 +/- 10 s, tau_4 = 414 +/- 9 s
- Accumulation profile parameters (a, tau_1, tau_1') =
a = 0.42 +/- 0.03, tau_1 = 131 +/- 7 s, tau_1' = 410 +/- 13 s
assumptions (3)
- domain assumption Superthermal UCN production in superfluid 4He via single-phonon conversion of 0.89 nm cold neutrons is the dominant production mechanism.
- domain assumption Absorption losses in 4He are negligible and upscattering at T <= 0.6 K is negligible; the superleak reduces 3He contamination to acceptable levels.
- domain assumption The number of UCN detected after extraction equals the number stored in the 14.2 L converter volume, without corrections for detector efficiency, transport losses, or the ~5% of UCN that cannot exit.
Cite this review
Pith. "Pith review of High-Density Ultracold Neutron Source for Low-Energy Particle Physics Experiments." pith.science (2026). https://pith.science/paper/URTIWKD6
@misc{pith2026250413030,
author = {Pith},
title = {Pith review of: High-Density Ultracold Neutron Source for Low-Energy Particle Physics Experiments},
year = {2026},
howpublished = {\url{https://pith.science/paper/URTIWKD6}},
note = {Machine review of arXiv:2504.13030}
}
abstract
SuperSUN, a new superthermal source of ultracold neutrons (UCN) at the Institut Laue-Langevin, exploits inelastic scattering of neutrons in isotopically pure superfluid $^4$He at temperatures below $0.6\,$K. For the first time, continuous operation with an intense broad-spectrum cold neutron beam is demonstrated over 60 days. We observe continuous UCN extraction rates of $21000\,$s$^{-1}$, and storage in the source with saturated $\textit{in-situ}$ density $273\,$cm$^{-3}$. The high stored density, low-energy UCN spectrum, and long storage times open new possibilities in fundamental and applied physics.
Figures
Forward citations
Cited by 4 Pith papers
-
A New High-Intensity Source for Ultracold Neutrons
The completed TUCAN He-II superthermal source with LD2 moderator yields up to 6.75(3)×10^5 UCN/s continuously and 1.34(1)×10^7 UCNs after 60 s accumulation, exceeding all other operating sources.
-
Initial results of the TRIUMF ultracold advanced neutron source
The TRIUMF TUCAN ultracold neutron source detected (9.3 +/- 0.8) x 10^5 UCNs in 60 s irradiations at 37 uA, with yields rising linearly with beam current.
-
Towards Precise Simulations and Inference for the Neutron EDM
GEANT4 simulations of the SuperSUN ultracold neutron source are paired with neural simulation-based inference to recover UCN loss parameters from time-of-flight spectra.
-
Concept of the UCN Source at the WWR-K Reactor (AlSUN)
A proposed superfluid-helium ultracold neutron source for the WWR-K reactor is estimated to reach up to 6e4 UCN per cubic centimeter in the source and 5e3 in experiments.
Reference graph
Works this paper leans on
-
[39]
Hydrogen impurities in DLC can significantly reduce its neutron optical potential. These DLC coatings are pre- pared with deuterated precursor chemicals, to maintain a high scattering length density despite impurities
-
[1]
(5) Here a is a weight parameter, analogous to c in Eqs
= [afa(t;τ1) + (1−a)fa(t;τ′ 1)]P iNiP i[afa(ti;τ1) + (1−a)fa(ti;τ′ 1)] . (5) Here a is a weight parameter, analogous to c in Eqs. (3) and (4). Overall normalization in Eqs. (4) and (5) is fixed by the data. The fit results for storage are c = 0.17± 0.02, τ3 = 117 s± 10 s, and τ4 = 414 s± 9 s. For accumulation, we obtaina = 0.42±0.03,τ1 = 131 s±7 s, and τ′...
-
[2]
Steyerl, Ultracold Neutrons (World Scientific, 2020)
A. Steyerl, Ultracold Neutrons (World Scientific, 2020)
work page 2020
- [3]
-
[4]
V. K. Ignatovich, The physics of ultracold neutrons (Clarendon Press, 1990)
work page 1990
-
[5]
C. Abel, S. Afach, N. J. Ayres, C. A. Baker, G. Ban, G. Bison, K. Bodek, V. Bondar, M. Burghoff, E. Chanel, et al. , Measurement of the permanent electric dipole moment of the neutron, Phys. Rev. Lett. 124, 081803 (2020)
work page 2020
-
[6]
F. M. Gonzalez, E. M. Fries, C. Cude-Woods, T. Bai- ley, M. Blatnik, L. J. Broussard, N. B. Callahan, J. H. Choi, S. M. Clayton, S. A. Currie, et al. (UCNτ Collab- oration), Improved neutron lifetime measurement with UCNτ, Phys. Rev. Lett. 127, 162501 (2021)
work page 2021
-
[7]
M. P. Mendenhall, R. W. Pattie, Y. Bagdasarova, D. B. Berguno, L. J. Broussard, R. Carr, S. Currie, X. Ding, B. W. Filippone, A. Garc´ ıa, et al. (UCNA Collabo- ration), Precision measurement of the neutron β-decay asymmetry, Phys. Rev. C 87, 032501 (2013)
work page 2013
Show all 49 references
-
[8]
Cronenberg, P
G. Cronenberg, P. Brax, H. Filter, P. Geltenbort, T. Jenke, G. Pignol, M. Pitschmann, M. Thalhammer, and H. Abele, Acoustic Rabi oscillations between gravi- tational quantum states and impact on symmetron dark energy, Nature Phys. 14, 1022 (2018)
2018
-
[9]
Jenke, J
T. Jenke, J. Bosina, J. Micko, M. Pitschmann, R. Sed- mik, and H. Abele, Gravity resonance spectroscopy and dark energy symmetron fields: qBOUNCE experiments performed with Rabi and Ramsey spectroscopy, Eur. Phys. J. ST 230, 1131 (2021), arXiv:2012.07472 [hep-ph]
2021 arXiv
-
[10]
Altarev, C
I. Altarev, C. A. Baker, G. Ban, G. Bison, K. Bodek, M. Daum, P. Fierlinger, P. Geltenbort, K. Green, M. G. D. van der Grinten, et al., Test of Lorentz invari- ance with spin precession of ultracold neutrons, Phys. Rev. Lett. 103, 081602 (2009)
2009
-
[11]
A. N. Ivanov, M. Wellenzohn, and H. Abele (qBounce), Tests of Lorentz-Invariance Violation in the Standard- Model Extension with Ultracold Neutrons in qBounce Experiments, in 8th Meeting on CPT and Lorentz Sym- metry (2020) pp. 118–121
2020
-
[12]
N. J. Ayres, G. Bison, K. Bodek, V. Bondar, T. Bouil- laud, E. Chanel, P.-J. Chiu, B. Clement, C. B. Crawford, M. Daum, et al. , Search for an interaction mediated by axion-like particles with ultracold neutrons at the PSI, New J. Phys. 25, 103012 (2023)
2023
-
[13]
G. Ban, J. Chen, T. Lefort, O. Naviliat-Cuncic, W. Saenz-Arevalo, P.-J. Chiu, B. Cl´ ement, P. Larue, G. Pignol, S. Roccia, M. Guigue, T. Jenke, B. Perrio- lat, and P. Schmidt-Wellenburg, Search for neutron-to- hidden-neutron oscillations in an ultracold neutron beam, Phys. Re...
2023
-
[14]
Golub and J
R. Golub and J. Pendlebury, The interaction of ultra-cold neutrons (UCN) with liquid helium and a superthermal UCN source, Physics Letters A 62, 337 (1977)
1977
-
[15]
Ageron, W
P. Ageron, W. Mampe, R. Golub, and J. Pendelbury, Measurement of the ultra cold neutron production rate in an external liquid helium source, Physics Letters A66, 469 (1978)
1978
-
[16]
Golub, C
R. Golub, C. Jewell, P. Ageron, W. Mampe, B. Heckel, and I. Kilvington, Operation of a superthermal ultra-cold neutron source and the storage of ultra-cold neutrons in superfluid helium 4, Zeitschrift f¨ ur Physik B Condensed Matter 51, 187 (1983)
1983
-
[17]
C. R. Brome et al. , Magnetic trapping of ultracold neutrons, Phys. Rev. C 63, 055502 (2001), arXiv:nucl- ex/0103003
2001
-
[18]
Baker, S
C. Baker, S. Balashov, J. Butterworth, P. Geltenbort, K. Green, P. Harris, M. van der Grinten, P. Iaydjiev, S. Ivanov, J. Pendlebury, D. Shiers, M. Tucker, and H. Yoshiki, Experimental measurement of ultracold neu- tron production in superfluid 4He, Physics Letters A308, 67 (2003)
2003
-
[19]
Zimmer, K
O. Zimmer, K. Baumann, M. Fertl, B. Franke, S. Mironov, C. Plonka, D. Rich, P. Schmidt-Wellenburg, H. F. Wirth, and B. van den Brandt, A Superfluid he- lium converter for accumulation and extraction of ul- tracold neutrons, Phys. Rev. Lett. 99, 104801 (2007), arXiv:0705.3960 [nucl-ex]
2007 arXiv
-
[20]
Zimmer, F
O. Zimmer, F. M. Piegsa, and S. N. Ivanov, Superther- mal source of ultracold neutrons for fundamental physics experiments, Phys. Rev. Lett. 107, 134801 (2011)
2011
-
[21]
Masuda, K
Y. Masuda, K. Hatanaka, S.-C. Jeong, S. Kawasaki, R. Matsumiya, K. Matsuta, M. Mihara, and Y. Watan- abe, Spallation Ultracold Neutron Source of Superfluid Helium below 1 K, Phys. Rev. Lett. 108, 134801 (2012)
2012
-
[22]
F. M. Piegsa, M. Fertl, S. N. Ivanov, M. Kreuz, K. K. H. Leung, P. Schmidt-Wellenburg, T. Soldner, and O. Zim- mer, New source for ultracold neutrons at the Insti- tut Laue-Langevin, Phys. Rev. C 90, 015501 (2014), arXiv:1404.3527 [physics.ins-det]
2014 arXiv
-
[23]
Ahmed, E
S. Ahmed, E. Altiere, T. Andalib, B. Bell, C. P. Bidinosti, E. Cudmore, M. Das, C. A. Davis, B. Franke, M. Gericke, et al. (TUCAN), First ultracold neutrons produced at TRIUMF, Phys. Rev. C 99, 025503 (2019)
2019
-
[24]
Bison, M
G. Bison, M. Daum, K. Kirch, B. Lauss, D. Ries, P. Schmidt-Wellenburg, G. Zsigmond, T. Brenner, P. Geltenbort, T. Jenke, et al., Comparison of ultracold neutron sources for fundamental physics measurements, Phys. Rev. C 95, 045503 (2017)
2017
-
[25]
Schmidt-Wellenburg, K
P. Schmidt-Wellenburg, K. Andersen, and O. Zimmer, Ultra cold neutron production by multiphonon processes in superfluid helium under pressure, Nuclear Instruments and Methods in Physics Research Section A: Acceler- ators, Spectrometers, Detectors and Associated Equip- ment 611...
2009
-
[26]
S. K. Lamoreaux and R. Golub, Angular distribution of ultracold neutrons produced by scattering of cold neu- 6 trons in superfluid 4He, Sov. Phys. JETP Lett. 58, 792 (1993)
1993
-
[27]
Golub, On the storage of neutrons in superfluid 4He, Physics Letters A 72, 387 (1979)
R. Golub, On the storage of neutrons in superfluid 4He, Physics Letters A 72, 387 (1979)
1979
-
[28]
Chanel, D
E. Chanel, D. Beck, J. Bl´ e, S. Degenkolb, C. Desalme, L. Dimmler, R. Georgii, M. H.M., T. Neulinger, and F. Waldherr, Characterization of SuperSUN phase I, part I, Institut Laue-Langevin (ILL) doi:10.5291/ILL- DATA.TEST-3284 (2023)
2023 doi
-
[29]
D. Wurm, D. H. Beck, T. Chupp, S. Degenkolb, K. Fier- linger, P. Fierlinger, H. Filter, S. Ivanov, C. Klau, M. Kreuz, et al. , The PanEDM neutron electric dipole moment experiment at the ILL, EPJ Web Conf. 219, 02006 (2019)
2019
-
[30]
Chanel, S
E. Chanel, S. Baudoin, M.-H. Baurand, N. Belkhier, E. Bourgeat-Lami, S. Degenkolb, M. van der Grinten, M. Jentschel, V. Joyet, M. Kreuz, et al. , Concept and strategy of SuperSUN: A new ultracold neutron con- verter, Journal of Neutron Research 24, 111 (2022)
2022
-
[31]
m-value
The “ m-value” of multilayer coatings used for neutron supermirrors is the factor by which the critical angle ex- ceeds that of Ni with natural isotopic composition
-
[32]
Degenkolb, M
S. Degenkolb, M. Kreuz, and O. Zimmer, A tapered tran- sition guide with irregular octagonal cross-section, Jour- nal of Neutron Research 20, 117 (2018)
2018
-
[33]
Plonka, P
C. Plonka, P. Geltenbort, T. Soldner, and H. H¨ ase, Rep- lika mirrors—nearly loss-free guides for ultracold neu- trons—measurement technique and first preliminary re- sults, Nuclear Instruments and Methods in Physics Re- search Section A: Accelerators, Spectrometers, Detector...
2007
-
[34]
A. P. Serebrov, A. Vasil’ev, M. S. Lasakov, E. Siber, A. N. Murashkin, A. I. Egorov, A. K. Fomin, S. V. Sbitnev, P. Geltenbort, and O. Zimmer, Replica neutron guides for experiments with ultracold neutrons, Technical Physics 62, 164 (2017)
2017
-
[35]
Zimmer, P
O. Zimmer, P. Schmidt-Wellenburg, M. Fertl, H. F. Wirth, M. Assmann, J. Klenke, and B. van den Brandt, Ultracold neutrons extracted from a superfluid-helium converter coated with fluorinated grease, Eur. Phys. J. C 67, 589 (2010)
2010
-
[36]
Yoshiki, H
H. Yoshiki, H. Nakai, and E. Gutsmiedl, A new superleak to remove He3 for UCN experiments, Cryogenics 45, 399 (2005)
2005
-
[37]
A. G. C. Chemicals Inc., Amorphous Fluoropolymer CYTOP, https://www.agc-chemicals.com/file.jsp? id=jp/en/fluorine/products/cytop/download/pdf/ CYTOP_EN_Brochure.pdf, accessed: 2024-03-12
2024
-
[38]
Neulinger, D
T. Neulinger, D. Beck, E. Connolly, S. Degenkolb, P. Fierlinger, H. Filter, J. Hingerl, P. Nordin, T. Saer- beck, and O. Zimmer, Ultracold neutron storage in a bot- tle coated with the fluoropolymer CYTOP, Eur. Phys. J. A 58, 141 (2022)
2022
-
[40]
The minimum total UCN energy for extraction is ∼ 15 neV higher than the lowest total UCN energy that can exist in the source, implying that approximately 5% of the UCN produced are unable to exit the source
-
[41]
Groshev, V
L. Groshev, V. Dvoretskij, A. Demidov, V. Lushchikov, S. Nikolaev, Y. Panin, Y. Pokotilovskij, A. Strelkov, and F. Shapiro, [in Russian] Aqueous and zirconium-hydride converters of ultracold neutrons. Neutron confinement in copper and glass vessels., Proc. All-Union conference...
1974
-
[42]
Neulinger, H
T. Neulinger, H. Filter, and O. Zimmer, Vertical time- of-flight spectroscopy of ultracold neutrons, Nuclear In- struments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 1059, 168947 (2024)
2024
-
[43]
Steyerl, H
A. Steyerl, H. Nagel, F.-X. Schreiber, K.-A. Steinhauser, R. G¨ ahler, W. Gl¨ aser, P. Ageron, J. Astruc, W. Drexel, G. Gervais, and W. Mampe, A new source of cold and ultracold neutrons, Physics Letters A 116, 347 (1986)
1986
-
[44]
Bison, W
G. Bison, W. Chen, P.-J. Chiu, M. Daum, C. B. Dooren- bos, K. Kirch, V. Kletzl, B. Lauss, D. Pais, I. Rien¨ acker, et al. , Time-of-flight spectroscopy of ultracold neutrons at the PSI UCN source, The European Physical Journal A 59, 215 (2023)
2023
-
[45]
D.-T. Wong, M. Hassan, J. Burdine, T. Chupp, S. Clay- ton, C. Cude-Woods, S. Currie, T. Ito, C.-Y. Liu, M. Makela, et al., Characterization of the new ultracold neutron beamline at the LANL UCN facility, Nuclear In- struments and Methods in Physics Research Section A: Accelera...
2023
-
[46]
Golub and S
R. Golub and S. K. Lamoreaux, Neutron electric-dipole moment, ultracold neutrons and polarized 3He, Physics Reports 237, 1 (1994)
1994
-
[47]
Ahmed, R
M. Ahmed, R. Alarcon, A. Aleksandrova, S. Baeßler, L. Barron-Palos, L. Bartoszek, D. Beck, M. Behzadipour, I. Berkutov, J. Bessuille, et al. (nEDM), A New Cryo- genic Apparatus to Search for the Neutron Electric Dipole Moment, JINST 14 (11), P11017
-
[48]
Degenkolb, P
S. Degenkolb, P. Fierlinger, and O. Zimmer, Approaches to high-density storage experiments with in-situ produc- tion and detection of ultracold neutrons, Journal of Neu- tron Research 24, 123 (2022)
2022
-
[49]
Zimmer and R
O. Zimmer and R. Golub, Ultracold neutron accumula- tion in a superfluid-helium converter with magnetic mul- tipole reflector, Phys. Rev. C 92, 015501 (2015)
2015
Reviewed August 16, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.