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Vocabulary flashcards covering the principles of ro-vibrational spectroscopy, selection rules, spectral branches, vibration-rotation interaction, and the method of combination differences.
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Ro-vibrational spectroscopy
The study of transitions in gas-phase molecules that involve simultaneous changes in both vibrational and rotational energy states.
Δv=±1
The vibrational selection rule for fundamental transitions in simple diatomic linear molecules like CO.
ΔJ=±1
The rotational selection rule for simple diatomic linear molecules, indicating that pure vibrational transitions (ΔJ=0) are forbidden.
P-branch
A series of peaks in the ro-vibrational spectrum where ΔJ=−1, resulting in lower wavenumbers relative to the center (Vibration−Rotation).
R-branch
A series of peaks in the ro-vibrational spectrum where ΔJ=+1, resulting in higher wavenumbers relative to the center (Vibration+Rotation).
Null gap
The empty space at the exact vibrational frequency (ν0) in a diatomic ro-vibrational spectrum caused by the forbidden ΔJ=0 transition.
P(J′′)
A transition label indicating the rotational level of the lower state is J′′ and moves to state J′′−1 (e.g., P(1) is J′′=1→J′=0).
R(J′′)
A transition label indicating the rotational level of the lower state is J′′ and moves to state J′′+1 (e.g., R(0) is J′′=0→J′=1).
Vibration-Rotation Interaction
A physical complication where the rotational constant (B) is not constant because it depends on the vibrational state (v) and average bond length (r).
B∝1/r2
The relationship stating the rotational constant is inversely proportional to the square of the bond length; as vibration increases bond length (r_1 > r_0), the constant decreases (B_1 < B_0).
R-branch Compression
A spectral effect of vibration-rotation interaction where line spacing decreases (lines bunch together) as J increases.
P-branch Dilation
A spectral effect of vibration-rotation interaction where line spacing increases (lines spread apart) as J increases.
Combination Differences
An analytical method used to isolate rotational constants (B0 and B1) by choosing pairs of spectral lines that share a common upper or lower state.
Δ2F′′(J)=4B0(J+1/2)
The expression for ground state combination differences derived from R(J−1)−P(J+1), where the gradient of the plot against (J+1/2) is 4B0.
Δ2F′(J)=4B1(J+1/2)
The expression for excited state combination differences derived from R(J)−P(J), where the gradient of the plot against (J+1/2) is 4B1.
Parallel Modes (Stretches)
Vibrational motion along the bond axis in linear polyatomic molecules (like HCN) where selection rules result in only P and R branches (ΔJ=±1).
Perpendicular Modes (Bends)
Vibrational motion at right angles to the bond axis in linear polyatomic molecules that allows ΔJ=0 transitions.
Q-branch
An intense spike in the center of the spectrum for perpendicular vibrational modes where all ΔJ=0 transitions occur at nearly the same frequency.
3n−5
The formula used to determine the degrees of vibrational freedom for linear polyatomic molecules.
3n−6
The formula used to determine the degrees of vibrational freedom for non-linear molecules.
Non-Linear Ro-vibrational Spectrum
A complex spectrum characterized by a dense forest of overlapping lines due to three independent rotational constants (A, B, and C).