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Flipping

Recently commercially available X-ray systems for laminography have a spatial resolution limited to hundred microns, which is not enough for modem multilayer electronic devices and assembles. Modem PCBs, flip-chips, BGA-connections etc. can contain contacts and soldering points of 10 to 20 microns. The classical approach for industrial laminography in electronic applications is shown in Fig.2. [Pg.569]

Figure Bl.4.9. Top rotation-tunnelling hyperfine structure in one of the flipping inodes of (020)3 near 3 THz. The small splittings seen in the Q-branch transitions are induced by the bound-free hydrogen atom tiiimelling by the water monomers. Bottom the low-frequency torsional mode structure of the water duner spectrum, includmg a detailed comparison of theoretical calculations of the dynamics with those observed experimentally [ ]. The symbols next to the arrows depict the parallel (A k= 0) versus perpendicular (A = 1) nature of the selection rules in the pseudorotation manifold. Figure Bl.4.9. Top rotation-tunnelling hyperfine structure in one of the flipping inodes of (020)3 near 3 THz. The small splittings seen in the Q-branch transitions are induced by the bound-free hydrogen atom tiiimelling by the water monomers. Bottom the low-frequency torsional mode structure of the water duner spectrum, includmg a detailed comparison of theoretical calculations of the dynamics with those observed experimentally [ ]. The symbols next to the arrows depict the parallel (A k= 0) versus perpendicular (A = 1) nature of the selection rules in the pseudorotation manifold.
B) SINGLET-TRIPLET SPIN-FLIP CROSS SECTION... [Pg.2047]

In a coupled spin system, the number of observed lines in a spectrum does not match the number of independent z magnetizations and, fiirthennore, the spectra depend on the flip angle of the pulse used to observe them. Because of the complicated spectroscopy of homonuclear coupled spins, it is only recently that selective inversions in simple coupled spin systems [23] have been studied. This means that slow chemical exchange can be studied using proton spectra without the requirement of single characteristic peaks, such as methyl groups. [Pg.2110]

It is known that multivalued adiabatic electronic manifolds create topological effects [23,25,45]. Since the newly introduced D matrix contains the information relevant for this manifold (the number of functions that flip sign and their identification) we shall define it as the Topological Matrix. Accordingly, K will be defined as the Topological Number. Since D is dependent on the contour F the same applies to K thus K = f(F),... [Pg.648]

The fact that there is a one-to-one relation between the (—1) terms in the diagonal of the topological matrix and the fact that the eigenfunctions flip sign along closed contours (see discussion at the end of Section IV.A) hints at the possibility that these sign flips are related to a kind of a spin quantum number and in particular to its magnetic components. [Pg.667]

In case of three conical intersections, we have as many as eight different sets of eigenfunctions, and so on. Thus we have to refer to an additional chai acterization of a given sub-sub-Hilbert space. This characterization is related to the number Nj of conical intersections and the associated possible number of sign flips due to different contours in the relevant region of configuration space, traced by the electronic manifold. [Pg.667]

The general formula and the individual cases as presented in Eq. (97) indicate that indeed the number of conical intersections in a given snb-space and the number of possible sign flips within this sub-sub-Hilbert space are interrelated, similar to a spin J with respect to its magnetic components Mj. In other words, each decoupled sub-space is now characterized by a spin quantum number J that connects between the number of conical intersections in this system and the topological effects which characterize it. [Pg.668]

In Section IX, we intend to present a geometrical analysis that permits some insight with respect to the phenomenon of sign flips in an M-state system (M > 2). This can be done without the support of a parallel mathematical study [9]. In this section, we intend to supply the mathematical foundation (and justification) for this analysis [10,12], Thus employing the line integral approach, we intend to prove the following statement ... [Pg.668]

If a contour in a given plane surrounds two conical intersections belonging to two different (adjacent) pairs of states, only two eigenfunctions flip sign—the one that belongs to the lowest state and the one that belongs to the highest one. [Pg.669]

In other words, surrounding the two conical intersections indeed leads to the flip of sign of the first and the third eigenfunctions, as was claimed. [Pg.672]

In Sections V and VII, we discussed the possible K values of the D matrix and made the connection with the number of signs flip based on the analysis given in Section IV.A. Here, we intend to present a geomehical approach in order to gain more insight into the phenomenon of signs flip in the Af-state system (M > 2). [Pg.672]

This algebra implies that in case of Eq. (111) the only two functions (out of n) that flip sign are and because all in-between functions get their sign flipped twice. In the same way, Eq. (112) implies that all four electronic functions mentioned in the expression, namely, the jth and the (j + 1 )th, the th and the (/c -h 1 )th, all flip sign. In what follows, we give a more detailed explanation based on the mathematical analysis of the Section Vin. [Pg.673]

In Sections VII and Vm, it was mentioned that K yields the number of eigenfunctions that flip sign when the electronic manifold traces certain closed paths. In what follows, we shall show how this number is formed for various Nj values. [Pg.673]

We briefly summarize what we found in this Nj = 5 case We revealed six different contours that led to the sign flip of six (different) pahs of functions and one contour that leads to a sign flip of all four functions. The analysis of Eq. (87) shows that indeed we should have seven different cases of sign flip and one case without sign flip (not surrounding any conical intersection). [Pg.675]

This conclusion contradicts the findings discussed in Sections V.A.2 and V.A.3. In Section V.A.2, we treated a three-state model and found that functions can n ver flip signs. In Section V.A.3, we treated a four-state case and found that either all four functions flip their sign or none of them flip their sign. The situation where two functions flip signs is not allowed under any conditions. [Pg.676]

Since for any assumed contour the most that can happen, due to C23, is that Yi2(s) flips its sign, the corresponding 2x2 diabatic mahix potential, W(s), will not be affected by that as can be seen from the following expressions ... [Pg.684]


See other pages where Flipping is mentioned: [Pg.415]    [Pg.300]    [Pg.300]    [Pg.958]    [Pg.975]    [Pg.1256]    [Pg.1339]    [Pg.1483]    [Pg.1542]    [Pg.1552]    [Pg.1570]    [Pg.1573]    [Pg.1574]    [Pg.1598]    [Pg.2105]    [Pg.2108]    [Pg.2110]    [Pg.608]    [Pg.608]    [Pg.636]    [Pg.648]    [Pg.653]    [Pg.654]    [Pg.657]    [Pg.666]    [Pg.668]    [Pg.668]    [Pg.671]    [Pg.672]    [Pg.672]    [Pg.673]    [Pg.675]    [Pg.675]    [Pg.676]   
See also in sourсe #XX -- [ Pg.88 ]




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180° Flip motion

AMPA receptor flip and flop RNA splicing in hippocampal principal cells

Application of FLIP Technology

Avoiding Flip-flops

Back-flip

Base flipping

Basic Flip-Flop Circuit

Bistable Flip-Flop

Bit flipping

Bond breaking spin-flip method

Bond, flipping

Bond, flipping rotation

C-FLIP

Candy flipping

Chair conformations and ring flipping

Chair flip

Charge-flipping method

Chemical flip-flop

Clocked flip-flop

Coin flip example, statistics

Conformational Inversion (Ring Flipping) in Cyclohexane

Conformational flip

Conformational flipping

Conformational ring-flip mechanisms

Conformations ring-flipping

Coupled cluster method spin flip

Cyclohexane barrier to ring-flipping

Cyclohexane ring flip

Cyclohexane ring-flipping

Cyclohexane, axial bonds barrier to ring flip

Cyclohexane, axial bonds rate of ring-flip

Cyclohexane, axial bonds ring-flip

D-type flip-flop

DANTE flip angle

Diradicals spin-flip method

Distribution coin flips

Double quantum spin flip rate

Double quantum spin flip rate constant

Effect of Not Initializing Flip-Flops

Electronic circuit, flip-flop

Elementary flip

Envelope flip mechanism

Envelope flip mechanism Subject inde

Exchange calculations ring-flips

FLIP option

FLIP unit

FLIP-FLOP

FLIP-FRAP

FLIPs

Falling-edge-triggered flip-flop

Flip Chip Bonding Technology

Flip angle

Flip angle adjustable one-dimensional

Flip angle adjustable one-dimensional NOESY

Flip angle calculation

Flip angle experiments

Flip angle resolution dependence

Flip angle selection

Flip bifurcation

Flip chip bonding

Flip chip issues

Flip chip issues solder bumps

Flip chip method

Flip chip on flex

Flip chip process

Flip chip pull test

Flip chip technology Reliability

Flip chips

Flip chips reliability issues

Flip chips solder joining

Flip chips with underfill

Flip flop falling edge

Flip flop inference

Flip flop signal value assignment

Flip flop state storage

Flip flop testing

Flip mechanism

Flip mirror

Flip process

Flip protons

Flip rule

Flip top caps

Flip, interface

Flip-Chip Arrangements

Flip-Flop Spin Diffusion

Flip-back pulse

Flip-bond model

Flip-chip applications

Flip-chip applications carriers

Flip-chip applications curing

Flip-chip applications isotropic conductive adhesives

Flip-chip applications process

Flip-chip applications underfill

Flip-chip applications using isotropic conductive adhesives

Flip-chip components

Flip-chip devices

Flip-chip devices reliability

Flip-chip devices silicon

Flip-chip devices stress-dissipating adhesives

Flip-chip devices underfilling

Flip-chip technology

Flip-chip underfill

Flip-chip-on-board

Flip-flap mechanism

Flip-flop chromatography

Flip-flop configuration

Flip-flop coordination

Flip-flop disorder

Flip-flop functions

Flip-flop hydrogen bond

Flip-flop initialization

Flip-flop interaction

Flip-flop interaction spin diffusion

Flip-flop kinetics

Flip-flop master-slave

Flip-flop mechanism

Flip-flop micro fuel cells

Flip-flop model

Flip-flop motion

Flip-flop movement, phospholipid

Flip-flop phenomenon

Flip-flop problem

Flip-flop rate

Flip-flop rate, phospholipid, membrane

Flip-flop reorientation

Flip-flop spectroscopy

Flip-flop spin interaction

Flip-flop term

Flip-flop transition

Flip-overs

Flip/flop diffusion rate

Flip/flop splice variants

Flipped orientation

Flipping a coin

Flipping coins

Flipping matrices

Flipping proportions

Fluorescence loss in photobleaching (FLIP

Hair Flip

Helicity flip

Histidine flipping

Hydrogen flip-flop

INDEX flip-chip applications

Inclination-flip bifurcation

Incoherent spin-flip

Injection Site Residues and Flip-Flop Pharmacokinetics

JK flip flop

Lasers spin flip Raman

Lipid flip-flop

Lipids flip-flop migration

Local bond flips

Magnetic phase transitions spin-flip

Membrane flip-flop

Modeling flip-flop

Molecule flipping

Momentum flip

Multiplexed flip-flop

Mutual spin flip interactions

Mutual spin-flips

N Molecules Flipping Between Two Compartments

Nuclear magnetic resonance spectroscopy spin-flips

Nuclear magnetic resonance spin-flips

Nuclear spin flip lines

Nuclear spin-flip

One Molecule Flipping Between Two Compartment Model

One-bond flip

One-bond flip mechanism

One-ring flip mechanism

Orbit-flip bifurcation

Orbit-flip homoclinic bifurcation

Period-doubling bifurcation (flip

Pharmacokinetics flip-flop

Phenyl ring flips

Photochemical flip

Poly ring flips

Polymer flip chip

Proton-flip experiment

Pulse Width (Flip Angle)

Pulse sequence selective spin-flip method

Pulse sequence spin-flip method

Rearrangement) bridge flipping

Rework of Underfill Flip-Chip Devices and Ball-Grid Array Packages

Ring flip of cyclohexane

Ring flipping

Ring-flip

Ring-flip energy barrier

Ring-flip molecular model

Ring-flip motion of poly(p-phenylene vinylene)

Ring-flip rates

Rising-edge-triggered flip-flop

Root flipping problem

Scattering with spin-flip

Semi-selective spin-flip method

Side-chain flips

Sign flips

Single quantum spin flip rate

Small flip-angle pulses

Solving proportions by multiplying or flipping

Spectroscopy of Spin-Flip Transitions

Spin flip lines

Spin flip scattering

Spin flip-flop

Spin flipping

Spin flips

Spin-Flip Raman Lasers (SFRL)

Spin-flip Raman processes

Spin-flip approach

Spin-flip approach bond breaking

Spin-flip approach method

Spin-flip approach system

Spin-flip collisions

Spin-flip dynamics

Spin-flip excitations

Spin-flip methods

Spin-flip narrowing

Spin-flip operators

Spin-flip pattern

Spin-flip process

Spin-flip strategy

Spin-flip temperature

Spin-flip transitions

Spin-flip, definition

Spin-flipped configuration

Tail flip

Three-state molecular system, non-adiabatic sign flip derivation

Three-state system sign flip derivation

Two-ring flip mechanism

Underfill flip-chip devices

V-FLIP

Vector flipping

Vesicles lipid flip-flop

Water flip-back

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