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Development, integration and use of an ultra-high-strength gradient system on a human-size 3 T magnet for small animal MRI

Kuan-Hung Cho, Sheng-Min Huang, Chang-Hoon Choi, Ming-Jye Chen, Hsuan-Han Chiang, Richard P. Buschbeck, Ezequiel Farrher, N. Jon Shah, Ruslan Garipov, Ching-Ping Chang, Hsu Chang, Li-Wei Kuo (+1 others)
2019 PLoS ONE  
The diffusion gradients were applied along readout (R), phase encoding (P) and slice (S) directions, respectively.  ...  It was found that the susceptibility values in the corpus callosum regions between the contra-lesional and ipsi-lesional sides were significantly different (p = 3.08×10 −47 ).  ... 
doi:10.1371/journal.pone.0217916 pmid:31158259 pmcid:PMC6546248 fatcat:fblwdyviifgibgqxfw7tyssfma

Page 287 of National Union Catalog Vol. 4, Issue [page]

1953 National Union Catalog  
A 53-660 Library Buschbeck, Erhard, 1889- see Vienna. Burgtheater. 175 ;i. e.  ...  Buschbeck, Erhard, 1889- a mg =e dns Burgtheater. Wien, E. Miiller, 1946. *Chronsiogieches Verzeichnis der von Raoul Aslan am Burgtheater base igre Rollen™: p. 164-;170, Asian, — 1886- 2. Vienna.  ... 

Observation of the muon inner bremsstrahlung at LEP1

J. Abdallah, P. Abreu, W. Adam, P. Adzic, T. Albrecht, R. Alemany-Fernandez, T. Allmendinger, P. P. Allport, U. Amaldi, N. Amapane, S. Amato, E. Anashkin (+329 others)
2008 European Physical Journal C: Particles and Fields  
1 . . . d 3 p N × i,j η i η j ( p i⊥ • p j ⊥ ) (P i K)(P j K) dN h d 3 p 1 . . . d 3 p N ( 3 ) where K and k denote again photon four-and threemomenta, P are the 4-momenta of the beam e + , e − and N charged  ...  from Low [9] with a modification suggested by Haissinski [22] : dN γ d 3 k = α (2π) 2 1 E γ d 3 p μ i,j η i η j ( p i⊥ • p j ⊥ ) (P i K)(P j K) dN μ d 3 p μ ( 2 ) where K and k denote photon four-and  ... 
doi:10.1140/epjc/s10052-008-0779-z fatcat:xqjdrtwpivaozfwm5gwrpfdj7y

In This Issue: COVID-19 commentaries and open call papers

Duncan Hilchey
2020 Journal of Agriculture, Food Systems, and Community Development  
Stearns, William P. Davenport, and Jennifer E.  ...  Providing planetary health diet meals to low-income families in Baltimore City during the COVID-19 pandemic, by Richard D.  ... 
doi:10.5304/jafscd.2020.101.036 fatcat:wvhuqwarnfdcrjgov4uww6fqd4

Di-jet production in γ γ collisions at LEP2

J. Abdallah, P. Abreu, W. Adam, P. Adzic, T. Albrecht, R. Alemany-Fernandez, T. Allmendinger, P. P. Allport, U. Amaldi, N. Amapane, S. Amato, E. Anashkin (+328 others)
2008 European Physical Journal C: Particles and Fields  
The variables sensitive to such a difference are [8] x + γ = jets (E jet + p z,jet ) part (E part + p z,part ) and x − γ = jets (E jet − p z,jet ) part (E part − p z,part ) , where 'part' corresponds  ...  An additional cut on the mean jets transverse momentum p T > 4 GeV/c allows a p T asymmetry of the reconstructed jets.  ... 
doi:10.1140/epjc/s10052-008-0777-1 fatcat:xev7sxsluvcjfms2x66hpozyku

Page 4609 of Psychological Abstracts Vol. 88, Issue 11 [page]

2001 Psychological Abstracts  
M., 32982 Kuhiz-Buschbeck, J.  ...  ., 33113 Kurtz, Richard M., 32607 Kurtz, Shelly L., 35095 Kurzweil, Edith, 34941 Kuschick, Mateus B., 33126 Kutnick, P., 35083 Kutsay, Sergey, 33224 Kuzis, Gabriela, 34167 Kvaal, Kari, 33570 Kvale, Alice  ... 

Page 299 of PMLA. Publications of the Modern Language Association of America Vol. 74, Issue 2 [page]

1958 PMLA. Publications of the Modern Language Association of America  
Richard Billinger.” WZ, tv, ix, 1-8. Boll. 11265. Cotet, P. “Les débuts d’un écrivain: Heinrich Béll.” EG, xu, 139-144. 11266. Dotzenrath, Theo.  ...  TLS, 4 July, p. 381. 11234. Woerner, Gert. “Fiir und wider das Christen- tum.” WuW, xu, 97-98. 11235. Zimmermann, Werner.  ... 

Evidence for an excess of soft photons in hadronic decays of Z0

J. Abdallah, P. Abreu, W. Adam, P. Adzic, T. Albrecht, T. Alderweireld, R. Alemany-Fernandez, T. Allmendinger, P.P. Allport, U. Amaldi, N. Amapane, S. Amato (+336 others)
2006 European Physical Journal C: Particles and Fields  
Sjöstrand and P. Sonderegger for useful discussions, and to Dr. B. French for detailed considerations of several aspects of this work.  ...  1 ...d 3 p N i,j η i η j −(P i P j ) (P i K)(P j K) dN hadrons d 3 p 1 ...d 3 p N (2) where K and k denote photon four-and three-momenta, P are four-momenta of beam e + , e − and of the N charged outgoing  ...  It has the same form as (2) with the scalar products of four-vectors −(P i P j ) being replaced by ( p i⊥ · p j⊥ ), where p i⊥ = p i − ( n · p i ) · n and n is the photon unit vector.  ... 
doi:10.1140/epjc/s2006-02568-8 fatcat:m5aqch5hcbbufma5ifqtwwgmvu

Page 841 of Psychological Abstracts Vol. 88, Issue 2 [page]

2001 Psychological Abstracts  
Philip, 4497 Kuhtz-Buschbeck, Johann P., 5112 Kukull, Walter A.. 5113 Kulik, Liat, 6040 Kulkarni, Shrinivas K., 3879 Kumar, G. S. Udaya. 5823 Kumar, Vinod, 5399 Kunde, Karen, 4921 Kung.  ...  Dean, 3139 Klopp, John, 5110 Kloster, Robert, 5472 Kluft, Richard P., og Kluger, Avraham N., 6183 Knapp, Samuel, 5888 Knei-Paz, Cigal, 5653 Knight, Bob G., 6235 Knight, R.  ... 

Measurements of CP-conserving trilinear gauge boson couplings WWV (V≡γ,Z) in e+e− collisions at LEP2

J. Abdallah, P. Abreu, W. Adam, P. Adzic, T. Albrecht, R. Alemany-Fernandez, T. Allmendinger, P. P. Allport, U. Amaldi, N. Amapane, S. Amato, E. Anashkin (+332 others)
2010 European Physical Journal C: Particles and Fields  
The respective background cross-sections 3 Defined as 3 2 λ 3 where λ 3 is the smallest eigenvalue of the sphericity tensor S αβ = i p α i p β i i |p i | 2 .  ...  A further pre-selection was made before applying the full selection using the IDA: for jj eν and jj μν candidates the 2 Defined as i θ i ·|p i | i |p i | where θ i is the angle made by the momentum p i  ... 
doi:10.1140/epjc/s10052-010-1254-1 fatcat:z7ncye4bj5b6zkcyu6sebrd5ye

Masses, lifetimes and production rates of Ξ− and Ξ¯+ at LEP 1

J. Abdallah, P. Abreu, W. Adam, P. Adzic, T. Albrecht, T. Alderweireld, R. Alemany-Fernandez, T. Allmendinger, P.P. Allport, U. Amaldi, N. Amapane, S. Amato (+336 others)
2006 Physics Letters B  
The following cuts were used to select the Ξ − andΞ + samples: • the χ 2 -probability of the fit had to exceed 1%; • the Ξ momentum, p Ξ , had to fulfill 1.2 < ξ < 4.2 where ξ = − ln x p and x p = p Ξ  ...  /p beam ; this corresponds to 0.015 < x p < 0.3 or 0.7 < p Ξ < 14 GeV/c; • the Ξ momentum had to point into the barrel region of the detector (| cos θ | < 0.85); • the decay radius of the Ξ in the xy plane  ... 
doi:10.1016/j.physletb.2006.06.029 fatcat:wy3vqtshszadbmdytjhi4vlmka

Correlations between polarisation states of W particles in the reaction e − e +→W − W + at LEP2 energies 189–209 GeV

J. Abdallah, P. Abreu, W. Adam, P. Adzic, T. Albrecht, R. Alemany-Fernandez, T. Allmendinger, P. P. Allport, U. Amaldi, N. Amapane, S. Amato, E. Anashkin (+328 others)
2009 European Physical Journal C: Particles and Fields  
N w = i w i is the sum of all event weights w i , and the event weights w are defined as w = p , where p is the W W purity factor, defined as in Sect. 2.4, for each bin of (cos θ W − , cos θ * 1 , cos  ...  The application of the weight factors p is described in the following section. 4 The momentum vectors are taken from the constrained kinematic fit.  ... 
doi:10.1140/epjc/s10052-009-1123-y fatcat:lrlq5dpqenaqha4xi3kuwu27yq

Search for one large extra dimension with the DELPHI detector at LEP

J. Abdallah, P. Abreu, W. Adam, P. Adzic, T. Albrecht, R. Alemany-Fernandez, T. Allmendinger, P. P. Allport, U. Amaldi, N. Amapane, S. Amato, E. Anashkin (+328 others)
2009 European Physical Journal C: Particles and Fields  
The likelihood ratio function used in this analysis is given by: L R = L S L B = P S (E γ ) P B (E γ ) . (3.1) The probability density functions (P i=S,B ) used to construct L R were produced from the  ...  In terms of the parameter p = (1/M D ) 3 , to which the n = 1 signal cross-section is proportional, the combined loglikelihood function of the Bayesian formula was practically parabolic. p is estimated  ... 
doi:10.1140/epjc/s10052-009-0874-9 fatcat:ur37brfdxnhkzjlklawvikakbi

A study of ${\mathrm{b}}\bar{\mathrm{b}}$ production in e+e− collisions at $\sqrt{s}=130$ –207 GeV

J. Abdallah, P. Abreu, W. Adam, P. Adzic, T. Albrecht, R. Alemany-Fernandez, T. Allmendinger, P. P. Allport, U. Amaldi, N. Amapane, S. Amato, E. Anashkin (+328 others)
2009 European Physical Journal C: Particles and Fields  
particle tracks for which p i · T > 0.  ...  Q F is defined: Q F ≡ i q i |p i · T| κ i |p i · T| κ , (5.2) where p i and q i are the momentum and charge of particle i, T is the thrust axis, κ is an empirical parameter, and the sum runs over all charged  ... 
doi:10.1140/epjc/s10052-009-0917-2 fatcat:646wqtbpxvb4pd4bty4ut5kzne

A study of the b-quark fragmentation function with the DELPHI detector at LEP I and an averaged distribution obtained at the Z Pole

J. Abdallah, P. Abreu, W. Adam, P. Adzic, T. Albrecht, R. Alemany-Fernandez, T. Allmendinger, P. P. Allport, U. Amaldi, N. Amapane, S. Amato, E. Anashkin (+328 others)
2011 European Physical Journal C: Particles and Fields  
The N representation of the fitted function given in (18) is: f (N) = p 0 p 1 (p 2 + N) (p 2 + p 3 + N + 1) + (1 − p 1 ) (p 4 + N) (p 4 + p 5 + N + 1) . (19) The Mellin transformed distribution of the  ...  = (p rec Fig. 3 (a) distribution of x p = (p rec.  ... 
doi:10.1140/epjc/s10052-011-1557-x fatcat:sbokwf3j2rg4fgd5cr6c7vn22y
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