Parameter set: ZGDCESGP
Pulse sequence: zgdcesgp
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Description:
This experiment is used to record a 1D 1H spectrum of all signals for RNA samples in H2O.
The pulse sequence employs water suppression by excitation sculpting with gradients. Excitation sculpting is a robust technique which uses a gradient echo sequence to achieve very efficient suppression of the strong water signal while retaining the desired signals of the RNA sample. Therefore, this sequence is well suited for recording a 1D proton spectrum over the full chemical shift range.
As an option, this pulse program can be used with decoupling for either the 13C or 15N atoms. In addition to the imino peaks (which can be observed with higher sensitivity using the na_zggpjrse), this spectrum also shows the aromatic proton signals (A:H2, C/U:H6 and A/G:H8) around 7.5 ppm. Flanking this region are the amino peaks of A:H61/H62, C:H41/H42 and G:H21/H22. The H1’ ribose signals together with the H5 aromatic signals of C and U appear typically in the range of 6 to 5 ppm and the remaining ribose signals (H2’, H3’, H4’, H5’1 and H5’2) are found between 5 and 4 ppm.
Some signals may not be observable, because they overlap with the suppressed water signal. The excitation sculpting 1D 1H spectrum is also used for proper chemical shift referencing of the 1H signals and to verify the amount and quality of the RNA and whether other wanted and unwanted components are present in the sample, such as buffer signals or impurities.
Literature:
T.-L. Hwang & A.J. Shaka, J. Magn. Reson., Series A 112 275-279 (1995)
Parameter set: NA_ZGGPJRSE
Pulse sequence: na_zggpjrse
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Description:
This experiment is used to record a 1D 1H spectrum of the imino region of RNA (~10-15 ppm). It features a jump return echo sequence for binomial water suppression with the added benefit of increasing the imino signal intensity by preservation of the water magnetization. Most imino peaks appear between 15 and 10 ppm, but some up- or down‑field shifted exceptions to this rule might occur for imino protons in non-helical regions. The signal intensity (I) in this a jump return experiment is modulated on the chemical shift (CS) according to the following equation: I = sin³((Pi*/2) *(CS-o1p)/(CNST19-o1p). Maximum intensity is observed at the chemical shift set by CNST19. This scheme efficiently preserves the water magnetization along +Z. This allows for the use of a short relaxation delay D1 (as the imino proton magnetization is restored via chemical exchange with water).
Due to exchange with water protons the linewidth and number of observable imino proton signals are highly dependent as temperature influences base-pair stability and exchange rates. It is therefore advisable to optimize the experimental temperature specifically for imino proton spectral region (typically between 283 and 308 K).
Literature:
Parameter set: ZGDCPR
Pulse sequence: zgdcpr
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Description:
This experiment is used to record a 1D 1H spectrum of all signals for RNA samples in D2O.
The pulse program uses presaturation of the water signal during the relaxation delay. This allows for very selective suppression of the water signal and allows detection of ribose 1H signals close to the water.
As an option, this pulse program can be used with decoupling for either the 13C or 15N atoms. Moreover, the 1H 1D spectrum is also used for proper chemical shift referencing of the 1H signals and to verify the amount and quality of the RNA and whether other components are present in the sample, such as buffer signals or impurities.
Parameter set: NA_NOESYESGPPH
Pulse sequence: na_noesyesgpph
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Description:
This pulse sequence uses excitation sculpting to suppress water. For RNA in H2O, the spectral widths should be chosen so that the correlation of the imino protons with the aromatic and ribose signals can be observed (26 ppm). For increased resolution in the indirect dimension, the frequency can be shifted (via CNST22) so that the spectral width can be reduced to 12 ppm.
Literature:
M.J. Thrippleton & J. Keeler, Angew. Chem. Int. ed. 42, 3938-3941 (2003)
Parameter set: NA_NOESYGPPHPR
Pulse sequence: na_noesygpphpr
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Description:
The NOESY with presaturation is useful for RNA samples in D2O where imino and amino protons are anyway invisible. It operates with minimal water suppression for the residual H2O signal. The absence of amino protons reduces spectral crowding in the region between 6 - 8 ppm, and thus is well suited for the sequential correlation of aromatic and H1’ /H2’ protons and identification of individual ribose spin systems. In combination with the 2D 1H1H NOESY – for all protons (in H2O), the H5-H6 correlations for base-paired cytidines serve as anchor points for the sequential assignment.
Literature:
M.J. Thrippleton & J. Keeler, Angew. Chem. Int. ed. 42, 3938-3941 (2003)
Parameter set: NA_SFNOESYSF2D
Pulse sequence: na_sfnoesysf2d
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Description:
The SOFAST-SOFAST NOESY uses selective pulses that only affect the imino proton region and leave the H2O magnetization unperturbed. This allows the use of short D1 delays (0.3-0.5 s). Since only imino protons are recorded in the experiment, the spectral width can be chosen small to increase the resolution. With O1 set to 12 ppm (the center of the imino region) and both spectral widths set to 6 ppm; the spectrum covers in both dimensions the essential range for the imino-to-imino signals from 9 to 15 ppm.
Literature:
Parameter set: NA_SFNOESY2D
Pulse sequence: na_sfnoesy2d
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Description:
The SOFAST NOESY excites all protons before the t1 time and the NOE mixing time. After the NOE transfer, only the selective pulses for the imino signals are used. This means that the spectrum shows the NOE cross peaks from all protons (in the direct dimension) to the imino protons (in the indirect dimension).
Literature:
Parameter set: NA_SFHMQCF3GPPH
Pulse sequence: sfhmqcf3gpph
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Description:
This experiment is used to record a 2D 1H15N correlation spectrum for imino protons. The SOFAST 1H15N HMQC uses selective 1H pulses that only affect the imino proton region and leave the H2O magnetization unperturbed. 1H15N correlations can be acquired most sensitively with the SOFAST HMQC because the inter-scan delay can be selected short and thus many scans can be accumulated in a short time. In general, 15 minutes (15N labeled RNA) or 18 hours (unlabeled RNA) should be sufficient for good S/N.
Literature:
P. Schanda and B. Brutscher, J. Biomol. NMR. 33, 199-211 (2005)
Parameter set: NA_SFHMQCGPPH
Pulse sequence: sf_mehmqcgpph
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Description:
This experiment is used to record a 2D 1H13C correlation spectrum for the aromatic H2, H6 and H8 signals. The SOFAST 1H13C HMQC uses selective 1H pulses that only affect the aromatic proton region and leave the H2O magnetization unperturbed. 13C-1H correlations can be acquired with particular high sensitivity with the SOFAST-HMQC because the relaxation delay can be selected short and thus many scans can be accumulated in a short time. In general, 5 h should be sufficient to acquire a high quality spectrum. For 1H13C correlations, the SOFAST 1H13C HMQC can only be used for the aromatic range (H2/H6 and H8), the remaining signals are too close to the water resonance. However, this region is the most important for RNA assignment and the experiment can be used to record the 13C-dimension with high resolution.
Literature:
P. Schanda and B. Brutscher, J. Biomol. NMR. 33, 199-211 (2005)
Parameter set: NA_HSQCETGPSP.4
Pulse sequence: hsqcetgpsp.4
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Description:
The experiment is used for 13C/1H correlations of all aromatic and ribose atoms. Plays a minor role in the detection of unlabeled RNA because the resolution is too poor. Helps when comparing different labeled RNAs. In addition, water suppression is very effective due to gradient selection. In general, 9 h should be sufficient to measure a good spectrum
Literature:
Parameter set: NA_DIPSI2ESGPPH
Pulse sequence: na_dipsi2esgpph
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Description:
The 2D 1H1H TOCSY experiment (Total Correlation Spectroscopy) is a two-dimensional NMR method used to identify through-bond correlations within a spin system, typically in coupled proton networks in small molecules, peptides or sugars. In contrast to COSY, which only reveals direct scalar couplings (J), TOCSY can reveal indirect couplings across entire spin systems - even if some nuclei are not directly coupled. COSY helps to establish connections between chemically bound protons, and TOCSY enables the identification of complete spin systems. For nucleic acids, TOCSY provides a cleaner spectrum to observe the aromatic cross signals of H5 and H6 in pyrimidines. The mixing time for the correlation can therefore be short. Unfortunately, TOCSY cannot be used to assign the proton spin system of the ribose because the coupling constant between H1' and H2' in canonical RNA is small and therefore the transfer of magnetization does not work well with the exception of a C2' endo conformation. In this case, the 3JH1'H2' coupling is at 8-10 Hz, and the signals are visible in this range. This pulse sequence also uses excitation sculpting to suppress water. Since only the non-exchangeable protons provide cross signals, the spectral width can be small, considering the frequency jump, with 9 ppm in the direct dimension and 6 ppm in the indirect dimension.
Literature:
M.J. Thrippleton & J. Keeler, Angew. Chem. Int. ed. 42, 3938-3941 (2003)
B. Simon & H. Koestler, J. Biomol. NMR 73, 155-165 (2019)
J. Furrer, F. Kramer, J.P. Marino, S.J. Glaser & B. Luy, J. Magn. Reson., 166, 36-49 (2004)
Parameter set: NA_HPDI
Pulse sequence: na_hpdi
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Description:
The hetero-TOCSY technique, which uses a combination of heteronuclear cross-polarization and homonuclear coherence transfer, has been shown to offer higher sensitivity and resolution compared to traditional approaches such as INEPT-RELAY or INEPT-TOCSY due to the simultaneous coherence transfer and the in-phase and absorptive cross-peaks. In addition, the small coupling between 31P and protons (<12 Hz) and the relative sensitivity of 31P provide advantages in the application of hetero-TOCSY over techniques such as HMQC-TOCSY.
Literature:
G.W. Kellogg & B.I. Schweitzer, J. Biomol. NMR 3, 577-595 (1993)
G.W. Kellogg, J. Magn. Reson. 98, 176-182 (1992)
G.W. Kellogg, A.A. Szewczak & P.B. Moore, J. Am. Chem. Soc. 114, 2727-2728 (1992)
Parameter set: NA_HPDINO
Pulse sequence: na_hpdino
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Description:
The advantage of 31P-NMR is the 100% natural abundance of the NMR-active isotope. Unfortunately, the dispersion of 31P resonances is very limited. The application of the 2D hetero-TOCSY-NOESY method provides an approach for the sequential assignment of 31P resonances associated with H6, H8 and ribose protons of neighboring nucleotides. By adding a NOESY step to hetero-TOCSY, the aromatic and ribose protons can be correlated with the 31P resonances without the need for isotopic labeling. For overlapping signals use the 3D pulse sequence na_hpdino3d.
Literature:
G.W. Kellogg & B.I. Schweitzer, J. Biomol. NMR 3, 577-595 (1993)
G.W. Kellogg, J. Magn. Reson. 98, 176-182 (1992)
G.W. Kellogg, A.A. Szewczak & P.B. Moore, J. Am. Chem. Soc. 114, 2727-2728 (1992)
Parameter set: NA_ROESYADESJSGPPH
Pulse sequence: na_roesyadesjsgpph
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Description:
2D 1H1H ROESY (Rotating-frame Overhauser Effect Spectroscopy) is an alternative NMR technique to 2D 1H1H NOESY and is also suitable for investigating the structure and dynamics of RNA and DNA molecules. Due to the pulse sequence, TOCSY artefacts are often present in the spectrum. With the EASY ROESY (Efficient Adiabatic SYmmetrized ROESY) approach, these TOCSY artifacts can be well suppressed using adiabatic spin-lock pulses used off resonance without loss of sensitivity. The advantage of ROESY is that the negative ROE signals can be easily distinguished from the positive signals due to chemical exchange.
Literature:
C.M. Thiele, K. Petzold & J. Schleucher, Chem. Eur. J. 15, 585-588 (2009)
J. Schleucher, J. Quant, S. Glaser & C. Griesinger, J. Magn. Reson A 112, 144-151 (1995)
Parameter set: NA_P31
Pulse sequence: zgig
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Description:
This experiment is used to record a 1D 31P spectrum of the RNA backbone phosphates. It includes 1H-decoupling during acquisition.
Parameter set: NA_HMBCGPL2NDWG
Pulse sequence: hmbcgpl2ndwg
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Processing
Description:
The HMBC shows HC correlations via the 2J(CH), 3J(CH) and 4J(CH) couplings. For nucleic acids, the experiment is used for the assignment of A:H2 to A:H8 in adenine as both nuclei show a sizable (5-12 Hz) 4J(CH) coupling to A:C4. The 1J(CH) correlation of A:H2 is suppressed by a low pass filter.
Literature:
Parameter set: NA_B_TROSYF3GPPH
Pulse sequence: b_trosyf3gpph.2
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Description:
This experiment is an alternative to record a 2D 1H15N correlation spectrum for imino protons. The 2D 1H15N BEST-TROSY uses selective 1H pulses that only affect the imino proton region and leave the H2O magnetization unperturbed. 1H15N correlations can be measured most sensitively with the BEST-TROSY because the interscan delay can be short and thus many scans can be accumulated in a short time. In general, 15 minutes (15N-labeled RNA) should be sufficient for good S/N. The TROSY experiment shows reduced T2 relaxation rates compared to the SOFAST-HMQC and allows for longer acquisition times and higher resolution in the 15N dimension. This is advantageous for larger RNAs.
Literature:
A. Favier & B. Brutscher, J. Biomol. NMR 49, 9-15 (2011)
E. Lescop, T. Kern & B. Brutscher, J. Magn. Reson. 203, 190-198 (2010)
Parameter set: NA_FHSQCF3GPPH
Pulse sequence: na_fhsqcf3gpph
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Description:
Another alternative for a 1H-15N correlation is the FHSQC, which is particularly suitable for protons that exchange rapidly with the solvent. It is usually used for recording a spectrum of both, the amino and the imino region.
Literature:
Parameter set: NA_B_TRHNNCOSYGPPH3D
Pulse sequence: na_b_trhnncosygpph3d
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Description:
The experiment is used to record 2D 1H15N spectra in which the imino proton is correlated with the A:N1 and U:N3, if the imino proton is involved in a stable, exchange-protected base-pair. The experiment is built up by two different magnetization transfers: First, the H-N INEPT transfers the magnetization from the imino proton to the hydrogen-bond donor nitrogen via the 1JN3H3 coupling. Subsequently, the N-N COSY transfers magnetization from the hydrogen-bond donor nitrogen to the hydrogen-bond acceptor nitrogen via 2JN1N3 coupling. Thereby, the HNN-COSY provides direct proof for hydrogen-bonds in Watson-Crick base-pairs.
Literature:
Parameter set: NA_B_SLRHNNCOSYGPPH
Pulse sequence: na_b_slrhnncosygpph
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Description:
The experiment is used to record 2D 1H15N spectra in which the aromatic A:H2 proton is correlated with the A:N1 and U:N3, if the A is involved in a stable, exchange-protected base-pair. Magnetization is transferred in two steps: 1) H-N INEPT via the 2JN1H2 coupling 2) N-N COSY via the 2JN1N3 coupling.
If the coupling constants are adapted, the LR HNN-COSY is also suitable to detect Hoogsteen interactions that involve the purine N7 side. Magnetization transfer to R:N7 is achieved starting on H8 via 2JN7H8 coupling.
Literature:
Parameter set: NA_HSQCF3GPNOWGXY
Pulse sequence: na_hsqcf3gpnowgxy
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Description:
The experiment is used to record 2D 1H15N spectra in which the imino and amino protons are correlated through space to nearby protons via NOE. The experiment uses the Carr-Purcell-Meiboom-Gill 1H-15N magnetization transfer for NH/NH2 to minimize losses due to exchange. During the mixing time d8, magnetization from the 15N-edited imino and amino protons to any nearby RNA protons takes place. Notably, the C:N4-H5 correlation is frequently visible for base-paired C residues, provided the water suppression is good. Careful optimization of O1P, SPW1/PHCOR9 and SPW11/PHCOR8 is recommended. The CPMG-NOESY allows reduction of the f1 spectral (SWF1) width via a frequency jump (CNST29) for advanced users. Care must be taken when folding the imino resonances into the amino spectral region to avoid overlap between imino diagonal peaks with imino-amino cross-peaks.
Literature:
L. Mueller, P. Legault & A. Pardi, J. Am. Chem. Soc. 117, 11043-11048 (1995)
F.A.A. Mulder, C.A.E.M. Spronk, M. Slijper, R. Kaptein & R. Boelens, J. Biomol. NMR 8, 223-228 (1996)
Parameter set: NA_LRHSQCF3GPPH
Pulse sequence: na_lrhsqcf3gpph
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Description:
With the long-range FAST-HSQC, the non-exchangeable aromatics H2 and H8 are correlated with the N1/N3 and N7/N8 nitrogen atoms via the 2JHN coupling. The experiment is based on the FAST-HSQC described above, whereby the excitation center is located on the aromatic and the HN transfer is significantly extended to 20 ms. It is advisable to record this experiment on 15N-only labeled samples, as 13C labeling speeds up T2 relaxation of H2/H8 due to dipolar interaction with 13C2/13C8.
Literature:
Parameter set: NA_LRSFHMQCF3GPPH
Pulse sequence: na_lrsfhmqcf3gpph
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Description:
In the LR-SOFAST-HMQC, the non-exchangeable aromatics H2 and H8 correlate with the nitrogen atoms via the 2JNH coupling. The experiment is based on the SOFAST-HMQC described above, with the excitation center located on the aromatic protons and the HN transfer significantly extended to 20 ms.
Literature:
P. Schanda and B. Brutscher, J. Biomol. NMR. 33, 199-211 (2005)
Parameter set: NA_SF15NXF
Pulse sequence: na_sf15Nxf
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Description:
This experiment records the 15N-filtered 1D 1H spectrum and the 15N-edited 1D 1H spectrum in an interleaved manner as a pseudo-2D experiment. Use the AU program “split” with the option "ipap" to separate the spectra after acquisition. The first and second spectrum correspond respectively to the 15N-filtered and 15N-edited spectrum.
Literature:
P. Schanda and B. Brutscher, J. Biomol. NMR. 33, 199-211 (2005)
Parameter set: NA_NOESYSFHMQCF3GPPH3D
Pulse sequence: noesysfhmqcf3gpph3d
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Description:
The 3D NOESY-HMQC expands the 2D imino-NOESY into the 15N dimension of imino nitrogens, thereby adding resolution. To minimize the number of pulses, the 15N dimension is recorded as an HMQC. The SOFAST (sf) acquisition scheme allows for short interscan delays, ultimately resulting in enhanced sensitivity. Folding of the 15N dimension is achieved via optimization of SWF2 and O3P and should be checked in 2D 1H15N SOFAST-HMQC spectra. When setting up a 3D experiment, pseudo-3D test spectra should be recorded for the F3-F2 and F3-F1 dimension combinations, respectively, by setting TDF1 or TDF2 to 1.
Literature:
P. Rossi, Y. Xia, N. Khanra, G. Veglia & G. Kalodimos, J. Biomol. NMR 66, 259 (2016)
P. Schanda and B. Brutscher, J. Am. Chem. Soc. 127, 8014 (2005)
Parameter set: H2
Pulse sequence: zg2h
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Description:
A 1D experiment for detection of the 2H signal. Used for measuring the splitting of the solvent signal in an aligned sample for RDC measurements.
Parameter set: NA_SFHMQCIA
Pulse sequence: na_sfhmqcia
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Description:
The experiment measures two 1H-15N SOFAST-HMQC spectra without 15N decoupling in the 1H dimension (F2). The inphase and antiphase components are recorded in an interleaved fashion and can later be separated. This prevents the increasing peak overlap due to coupling evolution. If the sample is also 13C-labeled, decoupling can be selected as an option.
Processing:
Literature:
Parameter set: NA_N_BTROSY
Pulse sequence: n_btrosy
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Description:
The 15N-detected BEST-TROSY is most useful for large RNA constructs, due to the lower relaxation of the 15N-magnetization, which allows higher resolutions. The 1H-detected BEST-TROSY is however more sensitive and should be used for smaller RNAs. The excitation is performed on the protons, and detected on the nitrogens. The experiment requires a cryoprobe due to its inherent insensitivity. For even better sensitivity use TXO cryoprobes, as these are optimized for detection of 13C and 15N.
Literature:
Parameter set: HSQCT1ETF3GPTCWG3D
Pulse sequence: hsqct1etf3gptcwg3d
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Description:
This experiment is used to record a series of 2D 1H15N correlation spectra in a pseudo 3D fashion with varying relaxation delay times for the determination of 15N-T1. The experiment uses a watergate sequence for solvent suppression and temperature compensation for the series of spectra. A VDLIST is needed to set the variable delay times (commonly includes 8 or more relaxation delays ranging from 0 to 1-2 s). Set TD for the F1 (pseudo) dimension to the number of delays (with the acquisition mode (FnMODE) to QF(no-frequency)).
Parameter set: HSQCT2ETF3GPTCWG3D
Pulse sequence: hsqct2etf3gptcwg3d
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Description:
This experiment is used to record a series of 2D 1H15N correlation spectra in a pseudo 3D fashion with varying relaxation delay times for the determination of 15N-T2. The experiment uses a watergate sequence for solvent suppression and temperature compensation for the series of spectra. A VCLIST is needed to set the variable loop counter (commonly includes 8 or more numbers, determining the T2 delays by the amount of loops over a single CPMG element (with length d31). The counter numbers are set from the minimum value of 1 to where C × d31 is around 100-200 ms. Set TD for the F1 (pseudo) dimension to the number of delays (with the acquisition mode (FnMODE) to QF(no-frequency)).
Parameter set: NA_HSQCTRETF3GPSITC3D.3
Pulse sequence: na_hsqctretf3gpsitc3d.3
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Description:
This experiment is used to record a series of 2D 1H15N correlation spectra in a pseudo 3D fashion with varying relaxation delay times for the determination of 15N-T1rho. The experiment includes temperature compensation for the series of spectra. A VDLIST is needed to set the variable delay times (commonly includes 8 or more relaxation delays ranging from 10 to 200 ms). Set TD for the F1 (pseudo) dimension to the number of delays (with the acquisition mode (FnMODE) to QF(no-frequency)).
Parameter set: NA_HSQCNOEF3GPWG3D
Pulse sequence: hsqcnoef3gpwg3d
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Description:
This experiment is used to record two 2D 1H15N correlation spectra in a pseudo 3D fashion, with and without proton saturation, for the determination of the 15N{1H}-hetNOE. The experiment uses a watergate sequence for solvent suppression. Set TD for the F1 (pseudo) dimension to 2.
Parameter set: NA_B_HSQCEXF3GP3D
Pulse sequence: na_b_hsqcexf3gp3d
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Description:
This experiment is used to measure ZZ exchange between different states of an RNA molecule. For a qualitative assessment of the exchange, a single 2D spectrum can be recorded at one relaxation delay. In this case, set TD1 to 1 and use only a single delay value in the VDLIST.
For quantitative determination of the 15N ZZ-exchange rates, the experiment records a series of 2D 1H-15N correlation spectra in a pseudo-3D fashion using variable relaxation delays. A VDLIST is required to define the delay times, typically consisting of eight or more values ranging from 0 to 1-2 s. Set TD for the F1 (pseudo) dimension to the number of delays specified in the VDLIST.
Parameter set: NA_NOESYF3GPPHXF19
Pulse sequence: na_noesyf3gpphxf19
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Description:
This experiment combines isotope filtering and editing schemes to separate signals according to whether the observed protons are attached to 15N or 14N nuclei. Four phase-cycling combinations are recorded in an interleaved fashion and stored in a single dataset. This results in all combinations of editing and filter steps in four different subspectra:
Spectrum A contains signals from all protons that are bound to 14N. Spectra B and C contain correlations between 15N-bound and 14N-bound proton resonances. These spectra are particularly useful for identifying NOESY cross-peaks as diagonal signals are suppressed. They contain the same information, with the F1 and F2 dimensions exchanged. The differences between them are mainly related to digital resolution and potential artifacts near the F1/F2 diagonal. Spectrum D contains signals from all 15N-bound protons.
The combination of isotope filtering and editing greatly simplifies the interpretation of NOESY spectra by separating different classes of cross-peaks into individual subspectra. However, these additional filter and editing elements result in a significant loss of sensitivity compared to a conventional NOESY experiment.
Literature:
G. Otting & K. Wuethrich, J. Magn. Reson. 85, 586 - 594 (1989)
Parameter set: NA_NOESYGPPHXF15N
Pulse sequence: noesygpphwgxf15N
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Description:
The 2D 1H1H NOESY sequence with a 15N x-filter in both dimensions. This removes the signal from 15N-bound protons in F1 and F2. For RNA, this means that all imino and amino proton signals are suppressed. Therefore, only NOE signals from aromatic and sugar protons are observed. The protons bound to 15N are eliminated using a purge element (Breeze 2000). The spectrum is similar to a NOESY in 100% D2O. Water suppression is achieved via a standard WATERGATE sequence.
Literature:
Parameter set: NA_HSQCETGPSP.4
Pulse sequence: hsqcetgpsp.4
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Description:
The experiment is used for the 1H13C correlations of all aromatic and ribose atoms. The experiment is optimized for large 13C bandwidth (broadband shaped pulses for all purposes on 13C). Experiments for recording only specific ribose or aromatic 1H13C correlations selective HSQC experiments are available (for C1’, C5’, C2/C6/C8 or C5), that offer higher resolution due to selective 1J(CC) decoupling.
Parameter set: NA_HSQCCTETGPSP
Pulse sequence: na_hsqcctetgpsp
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Description:
The experiment is used for the 1H13C correlation of all the ribose atoms. The cross-peaks appear as singlets in the F1 dimension because of a constant-time chemical shift evolution period in which the 13C-13C couplings are refocused. This enhances the resolution of the experiment, but decreases sensitivity due to T2 relaxation during the constant-time delay. The constant-time HSQC is very useful for measuring all ribose carbon C2’, C3’ and C4’ atoms with high resolution. If only C1’ or C5’ are of interest, the HSQC versions specialized for these two nuclei offer better sensitivity.
Parameter set: NA_SHSQCETGPSP_C1PRIME
Pulse sequence: na_shsqcetgpsp
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Description:
The experiment is used for the 1H13C correlation of the ribose C1’-H1’ atoms. The experiment uses shaped pulses on 13C and a selective 13C-decoupling (C2’-region).
Parameter set: NA_SHSQCETGPSP_C5PRIME
Pulse sequence: na_shsqcetgpsp
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Description:
The experiment is used for the 1H13C correlation of the ribose C5’-H5’ atoms. The experiment uses shaped pulses on 13C and selective 13C-decoupling (C4’-region).
Parameter set: NA_SHSQCETGPSP_C5
Pulse sequence: na_shsqcetgpsp
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Description:
The experiment is used for the 1H13C correlation of the aromatic C5-H5 atoms (C and U). The experiment uses shaped pulses on 13C and selective 13C-decoupling (range encompassing the C4-region and C6-region).
Parameter set: NA_SHSQCETGPSP_C2C6C8
Pulse sequence: na_shsqcetgpsp
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Description:
The experiment is used for the 1H13C correlation of the region of the aromatic C2-H2 atoms (A), the C6-H6 atoms (C and U) and C8-H8 atoms (A and G). The experiment uses shaped pulses on 13C and selective 13C-decoupling (encompassing the C5 (C and U) region).
Parameter set: NA_C6NOESYHSQCGP3D.2
Pulse sequence: na_c6noesyhsqcgp3d.2
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Description:
The 3D NOESY-HSQC expands the 2D aromatic-NOESY into the 13C dimension of aromatic carbons, thereby adding resolution. Folding of the 13C dimension is achieved via optimization of SWF2 and O2P and should be checked in 2D 1H13C HSQC spectra. When setting up a 3D experiment, 2D spectra should be recorded for the F3-F2 and F3-F1 dimensions, respectively, by setting TD1 or TD2 to 1.
Parameter set: NA_NOESY_SFHMQCHCH3D
Pulse sequence: na_noesy_sfhmqchch3d
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Description:
The 3D NOESY-HMQC expands the 2D aromatic-NOESY into the 13C dimension of aromatic carbons, thereby adding resolution. To minimize the number of pulses, the 13C dimension is recorded as an HMQC. The SOFAST acquisition scheme allows for short relaxation delays, ultimately resulting in enhanced sensitivity. Folding of the 13C dimension is achieved via optimization of SWF2 and O2P and should be checked in a 2D 1H13C SOFAST-HMQC spectrum. When setting up a 3D experiment, 2D spectra should be recorded for the F3-F2 and F3-F1 dimensions, respectively, by setting TD1 or TD2 to 1.
Literature:
P. Rossi, Y. Xia, N. Khanra, G. Veglia & G. Kalodimos, J. Biomol. NMR 66, 259 (2016)
P. Schanda and B. Brutscher, J. Am. Chem. Soc. 127, 8014 (2005)
Parameter set: NA_NOESY_SFHMQCHCHXF3D
Pulse sequence: na_noesy_sfhmqchchxf3d
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Description:
The xfilter 3D NOESY-HMQC is used to identify NOESY interactions between unlabeled binding partners and labeled RNA. It is also used to reduce signal overlap when assigning signals for selectively labeled RNA. To achieve this, a filter element is inserted before the t1 time, which suppresses signals bound to 13C or 15N.
A 3D NOESY-HMQC expands the 2D aromatic-NOESY into the 13C dimension of aromatic carbons, thereby adding resolution. To minimize the number of pulses, the 13C dimension is recorded as an HMQC. The SOFAST acquisition scheme allows for short relaxation delays, ultimately resulting in enhanced sensitivity. When setting up a 3D experiment, 2D spectra should be recorded for the F3-F2 and F3-F1 dimension combinations, respectively, by setting TD1 or TD2 to 1.
Literature:
A.L. Breeze, Prog. NMR Spectrosc. 36, 323-372 (2000)
P. Rossi, Y. Xia, N. Khanra, G. Veglia & G. Kalodimos, J. Biomol. NMR 66, 259 (2016)
P. Schanda and B. Brutscher, J. Am. Chem. Soc. 127, 8014 (2005)
Parameter set: NA_NOESYESGPPHXFED
Pulse sequence: na_noesyesgpphxfed
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Description:
A NOESY experiment with 13C/15N filtering in F1 and isotope editing in F2. The experiment is particularly useful for detecting ligand-RNA NOE contacts and for the analysis of selectively labeled RNA samples. Compared to a conventional NOESY experiment, the additional filtering and editing steps lead to a significant loss of sensitivity, typically requiring a substantially larger number of scans to obtain sufficient S/N.
The matched adiabatic pulse is generated using WaveMaker with the command wvm -a at the command line.
Literature:
Parameter set: NA_B_TRHNCOGP3D
Pulse sequence: na_b_trhncogp3d
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Description:
This 3D HNCO experiment is usually recorded as a 2D H/CO plane without chemical shift evolution of the 15N dimension. Imino protons (U:H3 and G:H1) of 13C-labeled RNA are directly correlated with U:C2 and U:C4 carbons or G:C2 and G:C6 carbons. If no C5 decoupling is applied, the U:H3C4 and G:H1C6 resonances appear as doublets in the indirect dimension, respectively.
Reference:
A. Favier & B. Brutscher, J. Biomol. NMR 49, 9-15 (2011)
E. Lescop, P. Schanda & B. Brutscher,J. Magn. Reson. 187 163-169 (2007)
T. Schulte-Herbrueggen & O.W. Sorensen, J. Magn. Reson. 144, 123 - 128 (2000)
Parameter set: NA_C_CNHSQC
Pulse sequence: na_c_cnhsqc
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Description:
In the CN-HSQC spectrum for imino groups, all nucleotides in the RNA can be observed, regardless of whether they are involved in hydrogen bonding or not. Using 13C direct detection, the correlation with the imino nitrogen is independent of exchange with water. Inserting a proton filter reverses the sign of the nitrogens with slow proton exchange rates (right spectrum). The filter can also be omitted (left spectrum); to do so, use the DNO_FILTER option. Due to the low sensitivity of the experiment, it is strongly advisable to use a cryogenic probe with a cooled 13C preamplifier. The experiment is even more sensitive when using a TXO cryoprobe in which the inner coil is optimized for 13C.
Literature:
Parameter set: NA_C_CN_IASQSP
Pulse sequence: na_c_cn_iasqsp
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Description:
The CN-HSQC for amino groups uses the in-phase/antiphase scheme for the virtual decoupling of A:1J(C6,C4) = 75 Hz and U:1J(C4,C5) = 55 Hz, so that a decoupled signal is recorded. Therefore, the following procedure is necessary for data processing
Parameter set: NA_TRHCCHCO3D
Pulse sequence: na_trhcchco3d
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Description:
TR-HCCH-COSY is designed for the assignment of adenine bases and links the assignment of A:C2/H2 to A:C8/H8 via the bridging carbons at adenine C4 and C5. For small RNAs, around 20 nucleotides, it is usually sufficient to run the F1/F3 plane as a 2D measurement.
Literature:
B. Simon, K. Zanier & M. Sattler, J. Biomol. NMR 20, 173-176 (2001)
Parameter set: NA_H5C5C4
Pulse sequence: na_h5c5c4
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Description:
The H5(C5)C4 experiment correlates the U/C:H5 with U/C:C4 through INEPT transfer steps and offers high sensitivity.
Parameter set: NA_H5C5C4N3N1
Pulse sequence: na_h5c5c4n3n1
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Description:
The long-range HNN-COSY version for C and U detects H-bond-mediated 2J-NN couplings across base-pairs in the absence of observable imino protons. The crucial NN-transfer happens during 4*d25 and is typically ~100 ms, which can lead to severe signal intensity loss for larger RNAs and should thus be optimized.
Literature:
Parameter set: NA_TRHCCNH3D
Pulse sequence: na_trhccnh3d
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Description:
The TRHCCNH is used to correlate the assigned imino protons U:H3 and G:H1 with the aromatic carbons U:C6 and G:C8. The pulse sequence is very insensitive because the INEPT transfers occur via weak coupling (~10 Hz) in combination with a long CC-TOCSY. Sensitivity is enhanced by the TROSY transfer. Nevertheless, many scans must be acquired to achieve sufficient S/N. Typically, only the F3/F2 plane is recorded, which requires 2 days of measurement time. This experiment is only suitable for smaller RNAs up to a maximum of 30 nucleotides. The experiment uses 15N- and 13C-TROSY steps. Due to this the signals in the 13C dimension (F2) are shifted by 1J(HC)/2 (G: 100Hz, U:90 Hz) and in 1H dimension (F3) by 1J(HN)/2 (47Hz).
Literature:
V. Sklenar, T. Dieckmann, S. E. Butcher & J. Feigon, J. Biomol. NMR, 7, 83 - 87 (1996)
The pulse sequence was developed by Frank Löhr (GUF), unpublished.
Parameter set: NA_HCNETGPSISP3D.2
Pulse sequence: na_hcnetgpsisp3d.2
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Description:
The HCN experiment is used to transfer assignments from the aromatic C6 and C8 carbons to the ribose C1′ carbons. To achieve this, the nucleobase correlations C/U:H6-C6-N1 and A/G:H8-C8-N9 are recorded simultaneously with the ribose correlations C/U:H1′-C1′-N1 and A/G:H1′-C1′-N9. Since the chemical shifts of C/U:N1 and A/G:N9 differ significantly among U, C, A and G residues, a simple 2D 1H/15N plane is often sufficient for resonance assignment in small RNAs.
For larger RNAs, it is recommended to record the aromatic and ribose correlations in two separate 3D experiments. For this purpose, use ZGOPTNS -DBASE for the aromatic correlations and ZGOPTNS -DSUGAR for the correlations to C1′. For both experiments, the 13C spectral width and O2P should be adjusted accordingly.
Literature:
V. Sklenar, R.D. Peterson, M.R. Rejante & J. Feigon, J. Biomol. NMR 3, 721 - 727 (1993)
Parameter set: NA_C_HCNCIASP
Pulse sequence: na_c_hcnciasp
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Description:
In the (H)CNC experiment, assignments of the aromatic C/U:H6-C6 and A/G:H8-C8 resonances are transferred to the sugar C1′ resonances, analogous to the HCN experiment. Direct 13C detection often enables the observation of additional correlations that may not be visible in proton-detected experiments.Due to the low sensitivity the experiment can only be performed efficiently on a cryogenic probe equipped with a cold 13C preamplifier. Even higher sensitivity can be achieved with TXO cryoprobes whose inner coil is optimized for 13C detection.
For virtual decoupling of the 1J(H1′C1)′ and 1J(C1′C2′) couplings, double inphase/antiphase elements are incorporated in an interleaved manner during the refocusing of the C1′-N1/N9 correlations. Data processing is performed using the AU program splitcomb.
The (H)CNC experiment is a 13C-TROSY variant in which the signals in the 13C dimension (F3) are shifted by 1J(HC)/2. A value of 100 Hz is typically used as a compromise for the different nucleotide types.
Literature:
V. Sklenar, R.D. Peterson, M.R. Rejante & J. Feigon, J. Biomol. NMR 3, 721 - 727 (1993)
The pulse sequence was developed by Frank Löhr (GUF), unpublished.
Parameter set: NA_HMQCNOESYHMQC4D
Pulse sequence: na_hmqcnoesyhmqc4d
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Description:
The 4D HCCH HMQC-NOESY-HMQC increases the resolution compared to the 3D NOESY experiments and helps in assigning the H1’-H6/H8 sequential walk. To ensure that the measurement time does not become too long, the experiment should be recorded using non-uniform sampling.
Literature:
J. Stanek, P. Podbevsek, W. Kozminski, J. PLavec, M.Cevev, J. Biomol. NMR 57, 1, (2013)
Parameter set: NA_SHCCHFLGPSP3D
Pulse sequence: na_shcchflgpsp3d
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Description:
Using the selective (H)CCH-TOCSY, all 13C signals in the ribose can be assigned. To achieve this, the magnetization of all ribose carbons is transferred to C1', which is detected in the F2/F3 dimensions. Since the chemical shifts of C2' and C3' are very similar, a TOCSY with a short mixing time (l1=1, d31=4.7 ms) is recorded first; here, only the correlation with C2' is visible. In a second 3D experiment, l1 is set to 3 (d31=14.1 ms), and all ribose carbon signals are visible. By comparing the two 3D spectra, C2' and C3' can be distinguished.
Literature:
Parameter set: NA_SHCCHFLGPSP3D2
Pulse sequence: na_shcchflgpsp3d2
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Description:
Using the selective (H)CCH-TOCSY, all 1H signals in the ribose can be assigned. To achieve this, the magnetization of all ribose protons is transferred to C1', which is detected in the F2/F3 dimensions. To reduce overlap the experiment can be recorded with a short mixing time (l1=1, d31=4.7 ms). Here, only the correlation to the H2' is visible. By setting l1 to 3 (d31=14.1 ms) magnetization will be transferred from all ribose protons (H2’,H3’,H4’ and H5’).
Literature:
Parameter set: NA_HCPETGPSI3D
Pulse sequence: na_hcpetgpsi3d
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Description:
The 3D HCP triple-resonance experiment correlates the ribose C3’-H3’, C4’-H4’ and C5’-H5’# resonances on either side of the phosphorus group by transfer of magnetization via 2,3J(CP) and 1J(CH) coupling constants.
Reference:
Parameter set: NA_HCPDIGPJR3D.2 (for QCI 1H{13C,15N,31P} probes)
Pulse sequence: na_hcpdigpjr3d.2
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Description:
The 3D HCP-TOCSY triple-resonance experiment extends the 3D HCP experiment with a CC-TOCSY (using a DIPSI3 sequence), in which the 13C magnetization is further relayed to the neighboring ribose nuclei through their 1J(CC) couplings. Efficient water suppression is accomplished using a 1-1 echo pulse sequence. This experiment includes 15N decoupling in F2 and F3 and requires a QCI 1H{13C,15N,31P} probe.
Reference:
Parameter set: NA_TRT1ETGPSITC3D
Pulse sequence: na_trt1etgpsitc3d
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Description:
This experiment is used to record a series of 2D 1H13C correlation spectra in a pseudo 3D fashion with varying relaxation delay times for the determination of 13C-T1 relaxation times. A VDLIST is needed to set the variable delay times (commonly includes 8 or more relaxation delays ranging from several ms to 1-2 s). Set TD for the F1 (pseudo) dimension to the number of delays.
Literature:
A. L. Hansen & H. M. Al-Hashimi, J. Am. Chem. Soc. 129, 16072-16082 (2007)
Parameter set: NA_TRTRETGPSITC3D
Pulse sequence: na_trtretgpsitc3d
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Description:
This experiment is used to record a series of 2D 1H13C correlation spectra in a pseudo 3D fashion with varying relaxation delay times for the determination of 13C-T1rho relaxation times. A VDLIST is needed to set the variable delay times (commonly includes 8 or more relaxation delays ranging from around 10 to 100-200 ms). Set TD for the F1 (pseudo) dimension to the number of delays.
Literature:
A. L. Hansen & H. M. Al-Hashimi, J. Am. Chem. Soc. 129, 16072-16082 (2007)
Parameter set: NA_SELT1RGPF22D
Pulse sequence: na_selt1rgpf22d
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Description:
T1ρ Relaxation dispersion (T1rhoD) is typically used to comprehensively quantify the parameters associated with chemical or conformational exchange on the microsecond-to-millisecond timescale. This window covers key structural refolding events in RNA at the individual base-pair level.
The experiment is designed to selectively excite a single peak. Therefore O2P and CNST30 need to be adjusted for every experiment, to achieve the excitation of the desired peak, based on its 1H and 13C chemical shifts. The rates of the exchange process accessible by T1rhoD are determined by the field strength of the field applied in the rotating frame, i. e., the “spin-lock”, during the relaxation delay and range from 100 to 2000 Hz for 13C. The spin-lock is applied in a series of different field strengths and offsets relative to the resonance under investigation. The apparent T2 relaxation times show a dispersion profile if this resonance is involved in an exchange process on the respective timescale. At the same time, a dispersion profile is observed at the same field strength but at a distinct offset, corresponding to the chemical shift of the exchanging conformational state of the resonance.
Literature:
Hansen, A.L., Nikolova, E.N., Casiano-Negroni, A.& Al-Hashimi, H.M., JACS 131, 3818 (2009)
Parameter set: NA_HSQCNOEGPSPWG3D
Pulse sequence: na_hsqcnoegpspwg3d
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Description:
This experiment is used to record two 2D 1H13C correlation spectra in a pseudo 3D fashion either with or without proton saturation during the relaxation delay, for the determination of the 13C{1H} heteronuclear NOE (hetNOE). Set TD for the F1 (pseudo) dimension to 2. The experiment uses WATERGATE for water suppression and is therefore optimal for aromatic protons.
Parameter set: NA_HSQCNOEETGPSP3D
Pulse sequence: na_hsqcnoeetgpsp3d
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Description:
This experiment is used to record two 2D 1H13C correlation spectra in a pseudo 3D fashion either with or without proton saturation during the relaxation delay, for the determination of the 13C{1H} heteronuclear NOE (hetNOE). Set TD for the F1 (pseudo) dimension to 2. Gradient selection enables detection of ribose proton signals for samples in H2O.
Parameter set: NA_HSQCGPIASP_C2C6C8
Pulse sequence: na_hsqcgpiasp
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Description:
The experiment measures two 1H13C HSQC spectra without 13C-decoupling in the proton dimension (F2). The inphase and antiphase components are recorded in an interleaved fashion and can later be separated during processing. This prevents the increasing peak overlap due to coupling evolution. If the sample is 15N-labeled, decoupling can be selected as an option.
Processing:
Parameter set: NA_HSQCGPIASP_C5
Pulse sequence: na_hsqcgpiasp
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Description:
The experiment measures two 1H13C HSQC spectra without 13C-decoupling in the proton dimension (F2). The inphase and antiphase components are recorded in an interleaved fashion and can later be separated during processing. This prevents the increasing peak overlap due to coupling evolution. If the sample is 15N-labeled, decoupling can be selected as an option.
Processing:
Parameter set: NA_HSQCGPIASP_C1PRIME
Pulse sequence: na_hsqcgpiasp
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Description:
The experiment measures two 1H13C HSQC spectra without 13C-decoupling in the proton dimension (F2). The inphase and antiphase components are recorded in an interleaved fashion and can later be separated during processing. This prevents the increasing peak overlap due to coupling evolution. If the sample is 15N-labeled, decoupling can be selected as an option.
Processing: