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When is a symmetric body-bar structure isostatic?
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2010GuestA.pdf6 Feb 2014: E r C2 Cn>2(/). C(b) b br b2 bnC0 1 1 1 1. ... 3) for body-bar framewor. E r i. C(b) b br bcC0 1 1 1. -
doi:10.1098/rspa.2006.1750
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/seffen2007b.pdf8 Jan 2008: Dimensionless. U ZU$12ð1Kn2=bÞa3=Ept5bx, y, z orthogonal coordinates within plate; z is normal to the middle surfacea dimensionless torsional rigidity equal to 2r(1Kn2/b)b, r modular ratios, equal ... sx ZE. ð1Kn2=bÞ ex Cney; sy ZEb. ð1Kn2=bÞ ey -
Quantum Control of the Tin-Vacancy Spin Qubit in Diamond
www-g.eng.cam.ac.uk/nms/publications/pdf/2021Debroux.pdf16 Dec 2021: Wrachtrup, and B. B.Zhou, Quantum Technologies with Optically InterfacedSolid-State Spins, Nat. ... Com-mun. 7, 13512 (2016). [26] B. B. Zhou, P. C. Jerger, V. -
March 2012, published 19, doi: 10.1098/rsta.2011.0347370 2012 Phil.…
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2012PTRSL.pdf3 Feb 2014: b) The quadrants from (a) are now reconnected but without changingthe corrugation strain. ... ax = a(1 e)(x b) b = ex1 e , (2.6). -
Weak localization in electric-double-layer gated few-layer graphene
www-g.eng.cam.ac.uk/nms/publications/pdf/Gonnelli_2017_2D_Mater._4_035006.pdf3 Aug 2017: BB. B. B. B 2. B, B ,. iWL. 2. ( ). ( ). (2). where:. ( ) ( ) ( / / )ψ= F z z zln 1 2 1. ... For the data in figure 4(a) (3LG), the Berry phase. is π and ( ) ( / ) ( /( ))δ π= ϕ ϕ e h FB, B , B 4 B B B2. -
J ElastDOI 10.1007/s10659-015-9520-y Buckling of Naturally Curved…
www-g.eng.cam.ac.uk/advancedstructures/files/pdf/2015JE.pdf10 Mar 2015: B B. Audolyaudoly@lmm.jussieu.fr. K.A. Seffenkas14@cam.ac.uk. 1 UMR 7190 Institut Jean Le Rond d’Alembert, Sorbonne Universités, UPMC Univ Paris 06, CNRS,75005 Paris, France. ... d0i (S), (13b). R(S, t) = 0 [B. (ω01. )2] R̂(S) ei τ , (13c). -
SE14 paper Dev of design methods of glass structures:Layout 3
www-g.eng.cam.ac.uk/gft/media/PG%20projects/Mauro%27s%20publication/SE14%20paper%20%20Dev%20of%20design%20methods%20of%20glass%20structures.pdf26 Jul 2010: a rb1 2. v v- =-. ,f ar b b. the load duration t. ... model uncertainties and dimensional variationsσar,b apparent residual stress ( 11MPa for annealed glass;. -
In Situ Observation of Low‐Power Nano‐Synaptic Response in Graphene…
www-g.eng.cam.ac.uk/nms/publications/pdf/2021Huitemp.pdf4 Aug 2021: 2019, 14, 35.[7] B. Govoreanu, G. S. Kar, Y.-Y. Chen, V. ... Chang, I. Ebong, B. B. Bhadviya, P. Mazumder, W. Lu, Nano Lett. -
nature nanotechnology…
www-g.eng.cam.ac.uk/nms/publications/pdf/Montblanch_2023SI.pdf25 Jul 2023: quantum dot. Phys. Rev. B 63, 161305 (2001).2. Kroutvar, M. et al. ... 142. Koehl, W. F., Buckley, B. B., Heremans, F. J., Calusine, G. & -
Hindawi Publishing CorporationJournal of NanomaterialsVolume 2012,…
www-g.eng.cam.ac.uk/nms/publications/pdf/Cole_JNanoMater2012.pdf9 May 2012: stan. ce (Ω. /sq. )1. CNT length (μm). (b). Figure 5: Opto-electronic performance. ... 6, no. 4, pp.677–682, 2006. [9] B. B. Parekh, G. Fanchini, G. -
Hasan_JPCC2008
www-g.eng.cam.ac.uk/nms/publications/pdf/Hasan_JPCC2008.pdf21 Jan 2009: E.; Avouris, P. Phys. ReV. B 1998, 58, 13870.(6) O’Connell, M. ... G.; Vamivakas, A. N.; Yin, Y.; Ünlü, M. S.; Goldberg,B. B.; Swan, A. -
Development of a universal stress sensor for graphene and carbon…
www-g.eng.cam.ac.uk/nms/publications/pdf/NatComm_2011.pdf29 Mar 2011: B A BA B B A. =. ( )( ) 0. ... Average. P55IMHM. P25MPP [25]. Group A [4]Group B [4]Group C [4]. -
arX iv:1 905. 0463 9v1 [ph ysic s.ap p-ph ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Muench2019.pdf14 May 2019: 3. (b). (c). Si3N4SiO2. SiO2. Si3N4. Ni/Au. SLG. SLG. Cr/Au. Si. ... Conductivity (. mS. ). VGate. (V). (b). p-p n-p. n-np-n. (a). -
Uniaxial strain in graphene by Raman spectroscopy: G peak ...
www-g.eng.cam.ac.uk/nms/publications/pdf/Mohiuddin_PRB_2009.pdf1 Jun 2009: Po. s(2. D). (cm. -1). Strain(%). B. ω2D/ε - 64cm-1/%. FIG. ... K. Swan, M. S. Unlu, B. B. Goldberg, M. A. Pimenta, J.
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