Raman Vocab 5 Flashcards

1
Q

occurs when two or more particles collide without any loss of energy

A

Elastic scattering

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2
Q

both conservation of momentum and conservation of kinetic energy are observed. This means that while the directions of the particles may change, the total kinetic energy of the system is always conserved

A

elastic collision

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3
Q

An elastic scattering process that occurs when photons of monochromatic radiation
with energy strikes a molecule, and the scattered radiation contains photons of the same energy as that of the incident radiation

A

rayleigh scattering

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4
Q

occurs when the collision of two or more particles is accompanied by a change in the internal state of the particles. the energy of the incident particles is not conserved; rather, some of the incident energy is gained or lost

A

inelastic scattering

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5
Q

part of the kinetic energy is changed to some other form of energy in the collision

A

inelastic collision

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6
Q

An inelastic scattering process that occurs when photons of monochromatic radiation with energy strike a molecule, and the scattered radiation contains photons of different energies
than that of the incident radiation. if change in E corresponding to ṽv lies in 0-3000 cm-1, then ṽv represents a change in the rotational/vibrational energy of the molecule, giving rise to a spectrum

A

raman scattering

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7
Q

The process by which the molecule gains energy during the inelastic Raman scattering collisions at the expense of the incident photons, resulting in Raman scattered photons of lower energy than that of the incident photons

A

stokes raman scattering

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8
Q

The process by which the photon gains energy during the inelastic Raman scattering collisions at the expense of the molecule, resulting in Raman scattered photons of higher energy than that of the incident photons,

A

anti-stokes raman scattering

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9
Q

The characterization of the energies of Raman vibrational modes by the magnitude of their wavenumber shift from the incident excitation energy, rather than their absolute
wavenumber. The use of wavenumber shifts to specify Raman vibrational energies insures that these bands are always plotted at identical energies, independent of the particular laser wavelength used in the experiment

A

raman wavenumber shift

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10
Q

mathematical relationship between two points that possesses both magnitude and direction

A

vector

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11
Q

The vector product of the distance separating two charges of equal magnitude and the magnitude of the charge

A

permanent dipole moment

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12
Q

magnitude of permanent dipole moment reflects

A

strength of polarity of bond

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13
Q

Result of the intense external electric and magnetic fields produced by the electromagnetic radiation of a laser inducing a separation of the electrons and protons in a molecule

A

induced dipole moment

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14
Q

The degree of deformation of the electron cloud of a molecule induced by an incident
electric field

A

polarizability

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15
Q

a 3 x 3 matrix that establishes a linear relationship between vectors.

A

tensor

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16
Q

the ratio of the intensity of the Raman scattered light polarized perpendicular to the X-Y plane to that of the scattered light polarized plane parallel to X-Y

A

depolarization ratio

17
Q

Raman vibration in which depolarization ratio = 0 .

A

completely polarized vibrational mode

18
Q

raman vibration in which 0 < ρ < 3/4.

A

polarized vibrational mode

19
Q

results in highly polarized raman bands

A

totally symmetric vibrations

20
Q

raman vibration in which ρ = 3/4

A

depolarized vibrational mode

21
Q

all antisymmetrical raman vibrations are

A

depolarized

22
Q

In a molecule that possesses a center of symmetry, molecular vibrations that are symmetric with regards to the center of symmetry are forbidden in the infrared spectrum, whereas molecular vibrations that are antisymmetric to the center of symmetry are forbidden in the Raman spectrum.

A

Rule of Mutual Exclusion

23
Q

the lasing medium is continuously pumped and continuously emits light. The emission can occur in a single resonator mode, i.e. single-frequency operation, or on multiple modes.

A

continuous wave laser

24
Q

the property of any laser where the optical power appears in a pulse train of a specified time duration at a specified repetition rate

A

pulsed lasers

25
Q

Common gas lasers used in Raman spectroscopy, often based on Ar+ or Kr+; generally high power consumption lasers as input energy must be used to first ionize the Ar or Kr atoms and then excite to high energy states for population inversion and lasing; CW or pulsed operation possible; high output power (10 W) possible; supports multiple important lasing wavelengths in blue, green and red spectral regions

A

ion lasers

26
Q

Common gas laser uses neutral atoms, not ions; low power consumption, high reliability; generally low output power (<100 mW); supports only a single red lasing wavelength, 632.8 nm.

A

He-Ne laser

27
Q

Solid state, doped semiconductors that function as a light-emitting diode, converting current into light. Highly efficient, with low power and cooling requirements, and a useful power range (0.1 – 1 W). Wide wavelength range available, primarily in the near-infrared region (670 – 860 nm). Most commonly used for Raman is 785 nm. Disadvantages include high divergence of the output beam, and multi-mode output that can lead to wavelength drift.

A

diode lasers

28
Q

A general class of instruments that collects, spectrally disperses, and reimages an optical signal. Widely used dispersive instrument used to optically isolate single wavelengths from a polychromatic source.

A

monochromator

29
Q

An instrument used for dispersing electromagnetic radiation into its component spectrum. Refers to a two-dimensional device in which the separated wavelengths are imaged simultaneously along a horizontal axis at the output focal plane. Can also refer to a dispersive instrument, e.g. a Czerny-Turner monochromator, in which the single element detector at the exit slit is replaced by a multichannel detector that records large segments of the spectrum at once in the focal plane of the instrument

A

spectrograph

30
Q

A spectrograph containing a single grating for dispersion. Single grating instruments are common, simple, and high throughput (f/# 4, T ~0.4) optical instruments; however, they have relatively poor laser line and stray light rejection capabilities (~10-5). Must be pair with a separate Rayleigh rejection filter for use in Raman spectroscopy.

A

single spectrograph

31
Q

A spectrograph in which two single grating monochromators are combined in series with a common intermediate slit. Uses “additive dispersion” in which the light is dispersed twice, leading to excellent stray light rejection properties (10-10 – 10-12). Disadvantage is relatively low throughput (f/# 8, T ~0.1); double spectrographs are also not as useful with multichannel detectors due to their high dispersion resulting in reduced spectral coverage.

A

double spectrograph

32
Q

A spectrograph with 3 gratings and 4 slits that is used for very high stray light rejection (10-12) and observation of small Raman shifts from the Rayleigh line (<100 cm-1). First two gratings act in “subtractive dispersion” mode as a specialized double pre-monochromator filter to efficiently eliminate the Rayleigh scattered light. Dispersion is done by the last (3rd) grating. Major disadvantage is very low overall optical throughput (f/# 6, T <0.1).

A

triple spectrograph

33
Q

Spectrograph based on a design that uses holographic transmission gratings coupled with holographic Raman notch filters. Very high optical throughput (f/# 1.8, T ~0.5) with very good stray light rejection (~10-11). Disadvantages are fixed wavelength and fixed resolution.

A

holographic spectrograph

34
Q

detector used in the UV/Vis spectral region that acts like a series of phototubes. The cathode and anode are biased by 400 – 2500 mV and separated by a series of intermediate dynodes, each progressively more positively biased, which provides an electron multiplication cascade. Overall: 106 amplification possible; however, have relatively low quantum efficiency (~1 – 10%).

A

Photomultiplier Tube

35
Q

multichannel detector used in UV/Vis/NIR spectral regions. Solid-state sensor with integrated circuit technology. Photons strike MOS-on-p-type Si capacitor; electron charge stored in wells; serial readout destroys accumulated charge; high quantum efficiency (90%) possible.

A

Charge Couple Device

36
Q

The averaging of signal over adjacent pixels, or even whole columns, in a multichannel detector to increase signal strength.

A

binning

37
Q

A two-grating tunable bandpass filter in which the 1st and 2nd stages have opposing dispersion directions; no net dispersion occurs, but this design strongly discriminates against the laser wavelength. Can be used as an effective Rayleigh laser line rejection filter.

A

subtractive pre-monochromator

38
Q

A multilayer dielectric or holographic filter that blocks the Rayleigh scattered wavelength while allowing both the Stokes and Anti-Stokes Raman shifted wavelengths to pass; notch filters have relatively narrow (5 – 10 nm) band widths with high absorbance (>106) at the design wavelength to block the Rayleigh scattered light; the notch filter will reject a high fraction of the Rayleigh wavelength but transmit wavelengths just a few nm’s away.

A

raman notch filters

39
Q

A multilayer dielectric filter with high absorbance (>106) at the laser wavelength to block Rayleigh scattered radiation, but also acts as a long pass filter to allow Stokes Raman shifted wavelengths to pass; generally provide the narrowest transition from high absorbance to high transmission for observation of Raman bands extremely close to the laser line. Also available as short pass filters to allow observation of Anti-Stokes Raman wavelengths.

A

raman edge filters