Modern Developments in X-Ray and Neutron Optics Episode 2 pptx

Modern Developments in X-Ray and Neutron Optics Episode 2 pptx

Modern Developments in X-Ray and Neutron Optics Episode 2 pptx

... following: F (x, y, z)=a 11 x 2 +signa 22 y 2 + a 33 z 2 +2a 12 xy +2a 13 xz +2a 23 yz +2a 14 x +2a 24 y +2a 34 z + a 44 + b 12 x 2 y + b 21 xy 2 + b 13 x 2 z + b 31 xz 2 + b 23 y 2 z + b 32 yz 2 =0 (2. 15) Here, ... 5.7) F x = −2x sign(ρ)  ρ 2 − x 2  (R − ρ)+sign(ρ)  ρ 2 − x 2  2 (2. 17) F y = 2( y − R) (2. 18) F z = −2z. (2. 19) Elliptical Pa...

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Modern Developments in X-Ray and Neutron Optics Episode 6 pptx

Modern Developments in X-Ray and Neutron Optics Episode 6 pptx

... described in (13.3). It is possible to make the measurement without changing anything in the LTP but instead by simply inclining the grating with respect to the optics table in order to obtain the ... spaced by 22 5 μm and rotated by 25 ◦ to minimize the overlap of the diffraction from adjacent holes in the measurement plane [8]. A back-illuminated, thinned, 16- bit EUV CCD came...

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Modern Developments in X-Ray and Neutron Optics Episode 1 docx

Modern Developments in X-Ray and Neutron Optics Episode 1 docx

... Kov´acs-Mezei, and L. Rosta 355 22 .1 Introduction 355 22 .2 Development and Investigation of Ni/Ti Multilayer Supermirrors for NeutronGuides 356 22 .2. 1NeutronGuides 356 22 .2. 2 Relation Between Crystalline ... Experiments 324 20 .4.1ExperimentsinVIS Region 324 20 .4.2ExperimentsinEUV Region 325 20 .4.3FutureExperiments withMFO 328 20 .5 Conclusions 328 References 329 21 CLE...

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Modern Developments in X-Ray and Neutron Optics Episode 3 doc

Modern Developments in X-Ray and Neutron Optics Episode 3 doc

... excited in the waveguide. Its thickness, i.e., the minimum thickness for efficient beam coupling D min , can be obtained by use of (6 .2. ) and (6.4): D min > λ 2 1  θ 2 c,1 − θ 2 c ,2 = 1 2 1  2 1 λ 2 − 2 2 λ 2 . ... 060701 (20 07) 12. S. Reiche, Nucl. Instrum. Methods A 429 , 24 3 (1999) 13. M. Abo-Bakr, R. Follath, A. Meseck, in Proceedings of the 27 th Intern...

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Modern Developments in X-Ray and Neutron Optics Episode 4 potx

Modern Developments in X-Ray and Neutron Optics Episode 4 potx

... ≈ ˜ Φ(kθ)exp  −iπ/4+ikθ 2 x /2  / √ λx, where ˜ Φ(kθ) ≈ d  sin(kθd /2) kθd /2 + cos(kθd /2) (kd /2)  θ c 2 − θ 2  , (6 .22 ) with two lateral plane waves, M 2 (x, y) (see (6 .21 )), entering into the vacuum gap ... 5 42, 24 8 (20 05) 26 . B.E. Allman et al., Neutron News 10, 20 (1999) 27 . M.R. Daymond, M.W. Johnson, Nucl. Instrum. Methods A 485, 606 (20 02) 28 . A.D....

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Modern Developments in X-Ray and Neutron Optics Episode 5 doc

Modern Developments in X-Ray and Neutron Optics Episode 5 doc

... ρ m · r)  d 2 A m (z) dz 2 − 2 jρ m,z dA m (z) dz −(ρ 2 m,x + ρ 2 m,z ) A m (z)+k 2 0 ¯εA m (z) + k 2 0 ΔεA m (z) 2 L L + S ∞  h=1 ,2, 3 sinc  hπ L L + S  cos(h G · r)  =0. (8 .24 ) We also ... (8 .22 ) ρ m,z = k cos θ in − mG sin ψ, (8 .23 ) with k =2 ¯ε 1 /2 /λ. An incident plane-wave E inc with wave vector ρ 0 is subdivided by X-ray diffraction inside the grating...

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Modern Developments in X-Ray and Neutron Optics Episode 7 doc

Modern Developments in X-Ray and Neutron Optics Episode 7 doc

... SPring-8 [ 12, 22 28 ] and APS [29 –35] facilities. For KB mirror fabrication at SPring-8, plasma chemical vaporization machining (PCVM) is employed for rough figuring, and elastic emission machining ... angle of incidence), following the N´evot–Croce formula [8]: R σ = R 0 exp  − 16π 2 σ 2 n h n l sin ϑ h sin ϑ l λ 2  . (16.6) In this formula, n l ,n h are the refractive indexes...

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Modern Developments in X-Ray and Neutron Optics Episode 8 doc

Modern Developments in X-Ray and Neutron Optics Episode 8 doc

... 33 Intensity gain 2, 8 92 7,078 7, 929 8,070 8,5 02 5,631 1,550 be neglected in most cases relative to the part containing the critical angle 2 cr f 1 ,2 . From these formulas, the following important ... 371, 307 (20 01) 7. A. Bjeoumikhov, N. Langhoff, R. Wedell, V. Beloglazov, N. Lebedev, N. Skibina, X-Ray Spectrom. 32, 1 72 (20 03) 8. C.A. MacDonald, W.M. Gibson, X-Ray Spectrom...

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Modern Developments in X-Ray and Neutron Optics Episode 9 potx

Modern Developments in X-Ray and Neutron Optics Episode 9 potx

... been possible to increase the number of layers from 150 to 1,000 and the m-value from m =2. 3to3.4. 22 .2 Development and Investigation of Ni/Ti Multilayer Supermirrors for Neutron Guides 22 .2. 1 Neutron ... revealed 22 Neutron Supermirror Development 357 0 123 45 0 20 40 60 80 100 Reflectivity of Ni / Ti supermirrors m =2 92% m =2. 5 90% m=3 87% m=3.6 78% m=4 72% Reflecti...

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Modern Developments in X-Ray and Neutron Optics Episode 10 doc

Modern Developments in X-Ray and Neutron Optics Episode 10 doc

... 300 ◦ C t Ni (nm) 1 .26 1 .26 1 .28 1. 32 1.33 1.34 t C (nm) 1.89 1.89 1. 92 1.98 1.99 2. 01 Λ (nm) 3.15 3.15 3 .23 .33. 32 3.35 ρ Ni (g cm −3 )8.98.98.98.58.58.0 ρ C (g cm −3 )2. 22. 22. 12. 02. 01.8 σ eff C-on-Ni (nm) ... together with a linear fit Fig. 23 .7. Grain size in the FeCo layers depending on the layer thickness 23 Stress Reduction in Multilayers Used for X-Ray and N...

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