what is a crystlline structure? Flashcards

1
Q

what is a crystallien structure?

A

asic pattern of atoms repeated over and over

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2
Q

braggs law

A

n (interner)lamda = 2d*sin(tetha)

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3
Q

why does bragg peaks occur

A

due to constructive interference

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4
Q

bigger atoms leads to more or less scattering

A

more due to more electrons that can ossilate which creates scattering

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5
Q

what is PDF

A

provides probability of finding pair of atoms at a distance r in the material

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6
Q

information in PDFs

A

peak position, peak intensity (bigger atoms = more intense peak), particle size

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7
Q

what is scattering

A

change in the direction of the beam

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8
Q

relation of Q and particle size in SAXS

A

inversilty related - larger Q = smaller particles

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9
Q

what is contrast in SAXS

A

the difference in electron density from the object to surroundings

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10
Q

Ephoton equals

A

binding + e kinetic

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11
Q

photo electric effect

A

photons in x ray beam has a certain amount of energy - if this energy is equal to or higher than the binding energy of electrons - electrons will absorb energy and leave surface of material - photoelectrons

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12
Q

XPS

A

surface sensitive. element specific. oxidation states. vacuum since electrons are easily trapped when interactig with e.g. air

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13
Q

why do we see 2 peaks for 2p data in XPS

A

P1/2, P3/2, peak splitting due to spin orbit coupling.

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14
Q

intensity of photoelectron

A

I = I_0 * e^d/lapda. lampda = inelastic mean free path, d = depth below surface.

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15
Q

what does µ, absorption coefficient, provide details about

A

the probability of absorption

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16
Q

bigger atoms in XPS. what does it do to binding energy

A

bigger nucleus = electrons more bound because of more proteins - more energy needed for unbinding the electron.

17
Q

what is scattering

A

photons in X ray has specific energy - when interacting with electrons in atom, the energy is reemitted by the electrons - sent out as scattered X ray

18
Q

when do we observe bragg peaks

A

when having speicifc wavelegnth that fits the distance between the atoms so that the scattered waves make construcutive interference

19
Q

what is XANES + pre edge

A

looks at transistions to unoccupied states. pre-edge privides knowledge about allowed and forbidden transistions.

20
Q

oxidations state and XANES

A

higher oxidation = less shielding = electrons are tighter bound why more energy is needed to unbind electrons

21
Q

µ is dependent on

A

the atoms in material.
distirbution of atoms
their bonding
lampda of X ray

22
Q

lambert beers law (XAS)1

A

I = I_0 * e^-µd
d = thickness of sample
I_0 = incoming intensity
I = outgoing intensity

23
Q

why is XPS element specific

A

looking at core electrons which are characteristic to the element.

24
Q

what is an auger electron (XAS)

A

when core electron is excited and leaves atom - creates vacancy inwhich a higher-lying electron can fall into. this electron can either emit flourescens or the excess energy can lead to an electron in outer shell leaving the atom. that outer electrin = auger electron

25
EXAFS
oscillations in µ. yields short range structure of materials. photoelectron has wavelike properties and can interact with the electrons in neighboring atoms which can be seen as point scatters.
26
compare gas and solid in how they would look in EXAFS
the closer structure, the more intereference, more oscialltions willbe observed in EXAFS. so solid = many oscillations. Gas = almost no oscillations liquid = in between
27
PDF vs EXAFS (similarities)
- fourier transforms - provides info on distance between atoms - bulk techniques (no surface sensitivity) - can measure solids, liquids, gasses
28
PDF vs EXAFS (differences)
- PDF = scattering, EXAFS. = absorption + scattering - EXAFS is more local - PDF can determine amorphous vs crystal. EXAFS cannot - EXAFS is element specific (since looking at core electrons). PDF is not
29
AFM vs SEM (conductivity)
AFM does not require conductive surface (therefore usefull no matter the sample). SEM require conductive surfaces to prevent build up of charge
30
contact mode vs tapping mode
contact mode: - constant interaction. Tip is dragged across the surface - rough interaction between sample + tip tapping mode': - good for biological / soft samples vibrating cantilever. - gentle interaction.
31
forces at the surface in AFM
electrostatic forces van der WALL forces columbic forces (repulsive. repulsion by electrons)
32
mica for AFM measurements
mica = a mineral has an even surface optically flat transparent free from contamination (when freshly cleaved)
33
SEM
Scanning electron microscopy. electron beam. vacuum, since we are detecting electrons surface sensitive
34
secondary electrons
inelastic electrons. sits at surface (top 10 nm) low energy electrons compared to the energy of the incoming beam. - when measured by detector, measured as current. more e- = more current at high point = appears brighter due to more electrons leaving
35
backscattered electron
elastic electrons. high energy electrons. able to see surface topography. The higher the atomic number of the investigated sample, the higher the amount of backscattered electrons
36
TEM
transmission electron microscopy. - trnasmitted electrons are measured. - thin samples - contrast in image comes from different electron density in sample. - vacuum
37
Characterisitc X-ray (SEM and TEM)
high energy electron from primary electron beam can kick a core electron out of the atom. To stabilize the atom, a higher-lying electron will drop down and fill the vacancy. This drop down will emit a X-ray photon. this photon will be specific for the element, why it is called charateristic X rays.
38
force curves AFM
force as a function of distance. Tell you about the forces between tip and surface of sample. tell furthermore about sample properties (stickyness)