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Overview of Commercially Available Femtosecond Lasers in … · 2017. 10. 21. · ]/[ tttI photo-disruption vaporisation photo-ablation coagulation 1 0 0 J/ cm ² 1 0 J/ cm ² 1 J

Some Basics - univie.ac.atZeeman Effect • normal Zeeman effect: S = 0, L = J ≠ 0 • split in 3 components components with mΔ J = 0 ( ) π components with mΔ J = 1 and +1 (±

Some Basics - univie.ac.atZeeman Effect • normal Zeeman effect: S = 0, L = J ≠ 0 • split in 3 components components with mΔ J = 0 ( ) π components with mΔ J = 1 and +1 (±

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THE PRESSURE METRIC FOR ANOSOV REPRESENTATIONScanary/arxiv4.pdf · formation space, let J (t) = J((0); (t)) then d dt t=0 J = 0 and d2 dt2 t=0 J >0: (1) Theorem1.3allows us to de

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Asymmetric system: E-I Symmetric system : S · j 0 j w 0 w x 1 x 2 x 1 x 2 j w j w 0 0 w j y 1 y 2 1 1 Asymmetric system: E-I Symmetric system : S y: Inhibitory unit strength inhibitory

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Single Out Put Transformer Trance Equations...SOPT (2) : Model 2 2 0 [0] j j j j j L j r j r r r l R L ω A n S nω µ µ ω ⋅ ≡ = = ⋅ ⋅ ⋅ ⋅ 1 0 1 1 [ ] V A AT n Lω ≡

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CONSUMER INSIGHTS servings chosen Breakdown of June 2017 … a… · CIN DWN CIIN ASN 0 10 20 0 0 0 0 0 10 20 0 0 0 0 D J * M M , M J J , - . / D J * M M , M J J , - . / D J J * M

CONSUMER INSIGHTS servings chosen Breakdown of June 2017 … a… · CIN DWN CIIN ASN 0 10 20 0 0 0 0 0 10 20 0 0 0 0 D J * M M , M J J , - . / D J * M M , M J J , - . / D J J * M

Hemwati Nandan Centre for Theoretical Studies Indian ...1 1 = σ 1 0 = 0. Similarly, the rotation tensor ω i j also satisﬁes uiω i j = 0 which leads to ω1 0 = ω 0 1 = 0. Therefore,

Hemwati Nandan Centre for Theoretical Studies Indian ...1 1 = σ 1 0 = 0. Similarly, the rotation tensor ω i j also satisﬁes uiω i j = 0 which leads to ω1 0 = ω 0 1 = 0. Therefore,

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