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Shaping Fibre for Optical Trapping

Shaping Fibre for Optical Trapping

Shaping Fibre for Optical Trapping. Steven Ross GERI-CEORG Supervisors: Prof. D. Burton, Dr. F. Lilley & Dr. M. Murphy . Introduction. Optical Trapping Theory Non “Classical” Methods Why Fibre Based Trapping? Fibre based Trapping Methods Methods for Shaping Fibre Ends Further work

By felton
(138 views)


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Single-beam chains

Single-beam chains

Single-beam chains. Single-beam chains. Being setup in TriggerMenuPython (Rasmus): In SingleBeam_v1.py and SingleBeam_v2.py First phase (SingleBeam_v1.py): MBTS commissioning with 32 L1 items + MBTS_A/MBTS_C HLT: taus more or less complete; rest incomplete Second phase (SingleBeam_v2.py):

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On Cavity Tilt + Gradient Change (Beam Dynamics)

On Cavity Tilt + Gradient Change (Beam Dynamics)

On Cavity Tilt + Gradient Change (Beam Dynamics). 2010.09.08 K. Kubo K. Kubo. Transverse effect of acc. field with cavity tilt. Acc. field E , length L, tilt angle q. beam. Transverse kick in the cavity: D pt = sin q eV. Edge (de)focus. exit. entrance. offset: y 0 -L sin q /2.

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Single-molecule force microscope

Single-molecule force microscope

Single-molecule force microscope. All biological motion, from cellular motility to replication and segregation of DNA, is driven by molecular-scale forces

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Single Particle Beam Dynamics Codes

Single Particle Beam Dynamics Codes

Single Particle Beam Dynamics Codes. Winni Decking DESY –MPY- HHH Workshop CERN 2004. Overview. Introduction Code repository Models used Programming philosophy Examples Summary This is a workshop contribution:

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Error gradient for a single unit network

Error gradient for a single unit network

2. Arbitrary feed-forward networks (multilayer perceptrons). Preliminaries:. Fix one of the inputs to 1, connect it to each unit that has a bias

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Nonlinear Beam Deflection - transverse force

Nonlinear Beam Deflection - transverse force

Nonlinear Beam Deflection - transverse force. Method of derivation: Curvature = Moment / Flexural Rigidity Elliptic Integrals Principle of Elastic Similarity End result: q, x, & y as a function of F F = K 1 q + K 2 *q 3 => F=F(q). y. EI. L. x. ds. dy. F 0. d. Y. dx. 1.

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Force-spectroscopy of single proteins

Force-spectroscopy of single proteins

Force-spectroscopy of single proteins. II: mechanical engineering in biological systems. Igor Demonstration of analysis with models of polymer elasticity. Reverse Engineering of the giant muscle protein titin. The elastic protein titin is the third filament of muscle.

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Force-spectroscopy of single proteins

Force-spectroscopy of single proteins

Force-spectroscopy of single proteins. I: Basic elements of protein mechanics. Are proteins exposed to mechanical forces in-vivo?. extracellular matrix. connector complex. P0. fibronectin. Schwann cell. Cytoskeleton: actin, etc. tenascin. cell. fascilin. Cadherin. NCAM.

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