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Changes in EPR spectra of an 15N isotopically labeled dinitroxide as J increases. A) Stick diagram calculated with CuNO 31 using ν = 9.852 GHz, g = 2.006, AN = 22.4 G, and Gaussian absorption line width of 0.2 G for J = 0, J = 0.5 AN, J = 2 AN, and J >> AN. For the AB pattern resulting from (mI(1),mI(2)) = (−1/2,1/2) or (1/2,−1/2) there are 4 lines centered at Bavg with positions and relative intensities as shown in Table 1. The resonances for (mI(1), mI(2)) = (1/2,1/2) and (−1/2,−1/2) are independent of J and occur at the positions labeled MI = 1 and −1, respectively. The changes in the positions of the lines as J increases are discussed in the text and shown with dashed lines for AB splitting pattern c. B) First derivative spectra calculated with <t>dynbirm</t> with the same parameters.
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Changes in EPR spectra of an 15N isotopically labeled dinitroxide as J increases. A) Stick diagram calculated with CuNO 31 using ν = 9.852 GHz, g = 2.006, AN = 22.4 G, and Gaussian absorption line width of 0.2 G for J = 0, J = 0.5 AN, J = 2 AN, and J >> AN. For the AB pattern resulting from (mI(1),mI(2)) = (−1/2,1/2) or (1/2,−1/2) there are 4 lines centered at Bavg with positions and relative intensities as shown in Table 1. The resonances for (mI(1), mI(2)) = (1/2,1/2) and (−1/2,−1/2) are independent of J and occur at the positions labeled MI = 1 and −1, respectively. The changes in the positions of the lines as J increases are discussed in the text and shown with dashed lines for AB splitting pattern c. B) First derivative spectra calculated with dynbirm with the same parameters.

Journal: Concepts in magnetic resonance. Part A, Bridging education and research

Article Title: Continuous wave electron paramagnetic resonance of nitroxide biradicals in fluid solution

doi: 10.1002/cmr.a.21426

Figure Lengend Snippet: Changes in EPR spectra of an 15N isotopically labeled dinitroxide as J increases. A) Stick diagram calculated with CuNO 31 using ν = 9.852 GHz, g = 2.006, AN = 22.4 G, and Gaussian absorption line width of 0.2 G for J = 0, J = 0.5 AN, J = 2 AN, and J >> AN. For the AB pattern resulting from (mI(1),mI(2)) = (−1/2,1/2) or (1/2,−1/2) there are 4 lines centered at Bavg with positions and relative intensities as shown in Table 1. The resonances for (mI(1), mI(2)) = (1/2,1/2) and (−1/2,−1/2) are independent of J and occur at the positions labeled MI = 1 and −1, respectively. The changes in the positions of the lines as J increases are discussed in the text and shown with dashed lines for AB splitting pattern c. B) First derivative spectra calculated with dynbirm with the same parameters.

Article Snippet: The MatLab-based program dynbirm is available upon request to the corresponding author.

Techniques: Labeling

Absorption EPR spectra (solid lines) of VI at 20°C in aqueous tris buffer recorded at A) 258 MHz and B) 1.09 GHz by rapid scan, and C) at 9.854 G by CW EPR. The spectrum in C) is the first integral of the CW spectrum. Spectra were obtained with RF or microwave power that is small enough that it does not impact the line shape. The dashed lines are simulations obtained with dynbirm using g = 2.0051 and AN = 44.95 MHz (16.05 G). Other parameters are discussed in the text.

Journal: Concepts in magnetic resonance. Part A, Bridging education and research

Article Title: Continuous wave electron paramagnetic resonance of nitroxide biradicals in fluid solution

doi: 10.1002/cmr.a.21426

Figure Lengend Snippet: Absorption EPR spectra (solid lines) of VI at 20°C in aqueous tris buffer recorded at A) 258 MHz and B) 1.09 GHz by rapid scan, and C) at 9.854 G by CW EPR. The spectrum in C) is the first integral of the CW spectrum. Spectra were obtained with RF or microwave power that is small enough that it does not impact the line shape. The dashed lines are simulations obtained with dynbirm using g = 2.0051 and AN = 44.95 MHz (16.05 G). Other parameters are discussed in the text.

Article Snippet: The MatLab-based program dynbirm is available upon request to the corresponding author.

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