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Olfactory neuroblastomas
1960
Cancer
.,* KENNETH D. DEVINE, M.D., AND Joun R. McDONALD, M.D.
LTHOUGH first described in 1924 in the
French literature by Berger, Luc, and Richard? ...
doi:10.1002/1097-0142(196001/02)13:1<205::aid-cncr2820130132>3.0.co;2-g
pmid:14428181
fatcat:7showsu7rnfn5gooxh7yuewtoy
Cancer in Childhood
1942
Radiology
Max Ritvo, JoHN D. HouGuton, EUGENE J. ...
., JOHN D. HOUGHTON,
TABLE I: DEATHS FROM CANCER AND OTHER MALIGNANT TUMORS BY AGE AND Sex (U
275
M.D., and EUGENE J. McDONALD, MD. ...
doi:10.1148/39.3.278
fatcat:rohl2r6bbjd27aye73mns3i4ye
B-ball Baryogenesis and D-term Inflation
[article]
1999
arXiv
pre-print
Evasion of thermalization and the ability to account for the observed baryon asymmetry requires a very low reheating temperature, which, it is argued, is a natural feature of presently favoured D-term ...
This is easily satified for the d=6 D-term inflation case. ...
In this case the flat directions are of even dimension [21] e.g. d=4 H u L-direction <ν L >=< φ o u > ; (H u L) 2 = 0 , (2) d=6 u c d c d c -direction (the d c QL and e c LL directions are similar) < ...
arXiv:hep-ph/9901453v3
fatcat:uhzurpftwvgctoure6vzm7gsxa
The Language of Driving
2013
Transportation Research Record
McDonald et al. ...
d (0 g)
41.68
−91.60
213.1
305.07
17.2
60
d (47 km/h)
d (0 g)
d (0 g)
41.68
−91.60
213.1
305.23
18.5
61
c (56 km/h)
d (0 g)
d (0 g)
41.68
−91.60
213.2
305.28 ...
doi:10.3141/2392-03
pmid:26203202
pmcid:PMC4507408
fatcat:6hazdbbfuzf3ffmyzprmajwpaa
F-term inflationQ-balls
2006
Physical Review D
In a previous paper we demonstrated the existence of Q-ball solutions of the field equations of the D-term inflation model [15] . ...
There are two classes of SUSY hybrid inflation model [1] , F-term [2] and D-term inflation [3] , depending on which part of the scalar potential drives inflation. ...
doi:10.1103/physrevd.73.043501
fatcat:n3zjvfq4ovfqtkls6tzyzmn53u
Observation of Breathers in an Attractive Bose Gas
[article]
2015
arXiv
pre-print
In weakly nonlinear dispersive systems, solitons are spatially localized solutions which propagate without changing shape through a delicate balance between dispersion and self-focusing nonlinear effects. These states have been extensively studied in Bose-Einstein condensates, where interatomic interactions give rise to such nonlinearities. Previous experimental work with matter wave solitons has been limited to static intensity profiles. The creation of matter wave breathers--dispersionless
arXiv:1509.06844v1
fatcat:wdk3nl5hdnhwrltcxob672w2zu
more »
... iton-like states with collective oscillation frequencies driven by attractive mean-field interactions--have been of theoretical interest due to the exotic behaviour of interacting matter wave systems. Here, using an attractively interacting Bose-Einstein condensate, we present the first observation of matter wave breathers. A comparison between experimental data and a cubic-quintic Gross-Pitaevskii equation suggests that previously unobserved three-body interactions may play an important role in this system. The observation of long lived stable breathers in an attractively interacting matter wave system indicates that there is a wide range of previously unobserved, but theoretically predicted, effects that are now experimentally accessible.
Distinguishing Higgs inflation and its variants
2011
Physical Review D
is the Ricci scalar with respect tog µν and dΩ dh = 1 2Ω ξ h hG 2 H M 2 p 2 − 2γ H 1 + γ H + 1 ξ h dξ h dt . (7) We can then rescale the fields using 5 dχ h dh = G 2 H Ω 2 + 6M 2 p Ω 2 dΩ dh 2 Ω 4 ; dχ ...
The parameterǫ is given bỹ ǫ = M 2 p 2 dφ dχ φ 2 dU dφ 1 U 2 (19) ≈ M 2 p 2 dφ dχ φ 2 4 φΩ 2 + L φ φ 2 (20) In the second expression 4 φΩ 2 is the tree-level contribution and L φ gives the approximate ...
This means that |D k | is small (from the requirement |R k | 2 + |D k | 2 = 1) and this gives the final line of Eq. (B-3). ...
doi:10.1103/physrevd.83.123522
fatcat:yf24ztroqzejtbrewph5sp2cxq
Robust real-time visual odometry for dense RGB-D mapping
2013
2013 IEEE International Conference on Robotics and Automation
KinectFusion, incorporating the following additions: (i) the integration of multiple 6DOF camera odometry estimation methods for robust tracking; (ii) a novel GPU-based implementation of an existing dense RGB-D ...
The score S for an algorithm A i given A and D is defined as S(A i , A, D) = n j E(A i , D j ) n m k E(A k , D j ) . (16) This ranking encapsulates the relative error each algorithm produces compared to ...
ICP+RGB-D for camera tracking. ...
doi:10.1109/icra.2013.6631400
dblp:conf/icra/WhelanJKLM13
fatcat:jjp5w3ug4zdp5ezqxxpp25gsee
CARDIOVASCULAR ACTIONS OF HUMAN ENDOTHELIN IN CONSCIOUS SHEEP
1989
Clinical and Experimental Pharmacology and Physiology
Scoggins, Campbell D. Spence, David G. Parkes, Michele McDonald, John D. Wade and John P. ...
D., Coghlan, J. P., Denton, D. A., Mills, E. H., Nelson, M. A., Whitworth, J. A. & Scoggins, B. ...
doi:10.1111/j.1440-1681.1989.tb01549.x
pmid:2663260
fatcat:5oxnjuhbkzehrisrkgj7747w54
Den Abandonment and Transitional Day Bed use by Black BearsUrsus americanusin Newfoundland
2014
Wildlife Biology
Hann, D. Jennings, R. Jennings, M. Mumma, D. O ' Leary, M. Payne, T. Porter and P. Tremblett for helping with bear captures. We thank helicopter pilots G. Aldie, J. Maloney, G. Pearcey and B. ...
Ursus americanus in Newfoundland Nathaniel D. Rayl , Todd K. Fuller , John F. Organ , John E. McDonald , Jr., Robert D. Otto and Shane P. Mahoney N. D. ...
McDonald, Jr., Environmental Science Dept, Westfi eld State Univ., 214A Wilson Hall Westfi eld, MA 01086, USA. -R. D. ...
doi:10.2981/wlb.00020
fatcat:ylkhr2ux5zcpnnsjv5ceh4s6uq
Real-time large-scale dense RGB-D SLAM with volumetric fusion
2014
The international journal of robotics research
By using a fused volumetric surface reconstruction we achieve a much higher quality map over what would be achieved using raw RGB-D point clouds. ...
We present a new SLAM system capable of producing high quality globally consistent surface reconstructions over hundreds of metres in real-time with only a low-cost commodity RGB-D sensor. ...
McDonald are with the Department of Computer Science, National University of Ireland Maynooth, Co. Kildare, Ireland. thomas.j.whelan@nuim.ie, johnmcd@cs.nuim.ie M. ...
doi:10.1177/0278364914551008
fatcat:alfgetv4w5dvzizngilbdshmcu
Deformation-based loop closure for large scale dense RGB-D SLAM
2013
2013 IEEE/RSJ International Conference on Intelligent Robots and Systems
In this paper we present a system for capturing large scale dense maps in an online setting with a low cost RGB-D sensor. ...
We provide benchmark results on a well established RGB-D SLAM dataset demonstrating the accuracy of the system and also provide a number of our own datasets which cover a wide range of environments, both ...
McDonald are with the Department of Computer Science, National University of Ireland Maynooth, Co. Kildare, Ireland. ...
doi:10.1109/iros.2013.6696405
fatcat:smolmv6cjzbaho6red2vw6eqlm
Highway Healthcare
2013
Proceedings of the Human Factors and Ergonomics Society Annual Meeting
accelerations over 0.1g an 'd' represents 0g of acceleration. ...
The concept of applying SAX to driving data was introduced in McDonald et al. (2012) . The steps for a segment of speed data are illustrated in Figure 1 . ...
doi:10.1177/1541931213571415
pmid:26500422
pmcid:PMC4613796
fatcat:dktpuxb6hbgshf4wzgdf5eo54m
A unitarity-conserving Higgs inflation model
2010
Physical Review D
The resulting unitarity-conserving action in the Jordan frame is given by S J = d 4 x √ −g − M 2 R 2 − ξH † HR + g µν D µ H † D ν H + 2ξH † H M 2 P g µν D µ H † D ν H − 3ξ 2 Ω 2 M 2 p g µν ∂ µ H † H ∂ ...
In the Jordan frame the action for Higgs Inflation (including the Higgs doublet and gauge fields) is S J = d 4 x √ −g − M 2 R 2 − ξH † HR + g µν (D µ H) † (D ν H) − 1 4 F µν F µν − V (|H|) , (1) where ...
doi:10.1103/physrevd.82.103525
fatcat:gktuxau7a5hglpkwdmdxsanipu
Gauge singlet scalars as cold dark matter
1994
Physical Review D, Particles and fields
The contours correspond toσ S−Ge = a) 1000kg −1 d −1 , b) 100kg −1 d −1 , c) 10kg −1 d −1 , d) 1kg −1 d −1 , e) 0.1kg −1 d −1 and f) 0.01kg −1 d −1 . ...
. < ∼ Ω S h 2 < ∼ 1.0, we require R < ∼ 1kg −1 d −1 . ...
doi:10.1103/physrevd.50.3637
pmid:10018006
fatcat:2xfdbveaangp5mpwu2gjc3c454
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