Cosy Experiments in Vnmr


I. COSY Experiment

II. Automatically Obtain a COSY Spectrum using Glide

III. Manually Setup for COSY ACQUISITION

IV. Acquire the COSY Spectrum and Save it for Processing


I. COSY Experiment


The COSY pulse sequence consists of an initial delay (d1) during period A that allows the magnetization to return to an equilibrium steady-state. This is followed by a pulse (p1) and delay (d2) that generates the spin-coupling information and allows that coupling to evolve. Finally, the resulting magnetization is examined with the pulse pw and the data acquired during time at. Long-range coupling information can be examined by adding a delay tau before and after the pw pulse. Additional pulses can be added to this sequence to 'relay' coupling information from one adjacent spin-coupled proton to the next in a spin system (sequence not shown). Important parameters in the COSY sequence are shown in the following table.


Observation pulse  pw                 90 degree pulse (will be automatically set to 90     
                                      degrees).                                            

Preparation pulse  p1                 90 degree pulse for normal COSY.  Use 45 degree for  
                                      COSY45 experiment.                                   

Relaxation Delay   d1                 set to 1-3*T1 (typically 0.6 to 3 secs).  Small d1   
                                      values can be used to speed the experiment, but      
                                      this can increase baseline artifacts.                

Evolution Delay    d2                 evolution time (t1 period).  d2 is automatically     
                                      incremented with each subsequent fid and should      
                                      always be equal to 0 to start.  The amount by which  
                                      d2 is incremented is determined by sw1.              

Data Acquisition   at                 acquisition time (t2 period).  Determined by sw and  
Time                                  the number of acquired data points in the            
                                      acquisition dimension (np).                          

Spectral Width     sw, sw1            spectral width (for COSY spectra, sw1 should always  
                                      = sw).  sw determines spectral width in the          
                                      acquisition dimension, while sw1 controls the        
                                      spectral width in the time-incremented dimension.    

Number of Time     ni                 number of t1 increments.  Set ni=128 for             
Increments (or                        low-resolution, 192-256 for medium resolution,       
fids)                                 400-512 for very high resolution.  ni may be         
                                      further decreased (e.g., 64-96) if speed is          
                                      essential.                                           

Coupling delay in  tau                propagation time for long-range COSY (relay = 0)     
long-range COSY                       and for relayed COSY (relay > 0)                     

Relayed-COSY       relay              number of relays to be performed; if relay = 0, a    
spectra                               normal absolute value COSY is performed; if relay =  
                                      1, a relay-COSY is performed; if relay = 2, a        
                                      DOUBLE-RELAY-COSY is performed.                      

Calculate          time               time will calculate the overall time required to     
Experiment Time                       acquire the 2d spectral data.  Allow about 5 extra   
                                      minutes for disk-preparation before acquisition.     

II. Automatically Obtain a COSY Spectrum using Glide

You can aqcuire a COSY spectrum automatically under GLIDE, or you can choose to obtain the COSY spectrum manually.

TO ACQUIRE THE SPECTRUM USING GLIDE: Click on Glide on the menu bar. Click on Experiment & Solvent. Choose Run proton and Cosy from the Experiment menu. Click DO. Then click the GO icon. That's it. The spectrometer will run a proton spectrum, optimize the sweep width, and then run a quick COSY experiment. The proton and cosy spectra will then be plotted. This will take about 25-30 minutes. DO NOT interfere with the spectrometer until plotting is complete. After the COSY spectrum has been plotted, you can save the data, re-process and replot as you wish, using the commands shown below.


III. Manually Setup for COSY ACQUISITION

A. Acquire a Proton Spectrum

The first step in setting up for a COSY spectrum is to acquire a proton spectrum of the sample and optimize the spectral width. Take a 1H NMR spectrum of the sample in the normal way. After data acquisition is finished, display the full spectrum (all 15 PPM) and put up two cursors. Bracket the left-most and right-most peaks in the spectrum with the cursors, leaving about 0.5 PPM of noise between each cursor and the nearest peak. Next, type movesw. movesw will adjust the spectral width SW and the transmitter frequency to correspond to the region defined by the two cursors. WARNING: DO NOT TYPE movesw MORE THAN ONCE IN THE SAME EXPERIMENT WITHOUT RE-ACQUIRING THE SPECTRUM.


Optimize Sweep     movesw             movesw will narrow the sweep width to the region     
Width                                 defined by the current position of the left and      
                                      right cursors.  The transmitter frequency (tof)      
                                      will be centered at the middle of the two cursors.   

After typing movesw, you may see a message that the number of points and sweep width will not give optimum signal to noise. This is normal on the Gemini, which lacks filters for best S/N at all sweep widths. Once the sweep width and transmitter frequencies have been set with movesw, you can begin to setup for a COSY experiment. The next step is to move these new acquisition parameters into the 2D workspace.


B. Move Acquisition Parameters and Setup COSY Pulse Sequence

VNMR allows you to acquire spectra in several workspaces that are called experiments. You can have up to nine on the UNIX workstations. Experiments can be used to run simple 1D spectra, arrayed spectra (T1 measurements, NOE difference, DEPT, Kinetics, etc.), or 2-, 3-, or 4-dimensional NMR spectra.

Once you have defined the optimum spectral window for the COSY experiment by taking a simple proton spectrum and narrowing the sweep width with movesw, you need to move these new parameters from the current experiment (exp1) to a new experiment, which will be used to acquire and process the COSY spectrum. Move the acquisition parameters from the proton experiment (exp1) to experiment 2 (exp2) by typing mp(1,2). This will copy the current acquisition parameters into exp2. Next, join exp2 by typing jexp2.

Once the 1D proton parameters have been copied into exp2, they can be transformed into the acquisition parameter set suitable for acquiring a COSY spectrum simply by typing cosy. cosy will load the pulse sequence required for to obtain a COSY spectrum, and will convert the optimized 1D parameters into the 2D parameter set. These commands are summarized in the following Table.


Join a different   jexpn              jexpn, will allow you to acquire, process and        
experiment                            display spectra in a different experiment.  n can    
                                      be 1 to 9.  The command will not work if the         
                                      experiment you want to join doesn't exist.           

move parameters    mp(n,m)            mp will copy all acquisition and processing          
to a different                        parameters from expt. n to expt. m., where n and m   
expt.                                 can be 1 to 9.  NOTE:  mp DOES NOT COPY THE FID!.    

Setup for COSY     cosy               cosy will transform the 1D proton acquisition        
                                      parameters into a parameter set suitable for         
                                      acquisition of a 2D COSY spectrum.                   

C. Adjust COSY Parameters for Desired Resolution and Time

Bear in mind that all users of the Gemini-300 are limited to one-hour. The Gemini can sometimes perform an adequate COSY experiment in this time. The Gemini will setup COSY acquisitions that require from 15 minutes to an hour or more. Processing of the spectra can have a tremendous influence on the quality of the result, i.e., a 10 min COSY spectrum, appropriately processed, may look far better than a 2-hour COSY spectrum that was not properly transformed.

Recognize that appropriate POST-processing of even marginal spectra can result in dramatic (orders of magnitude) improvements in sensitivity and resolution. Hence, long acquisitions are often not necessary to obtain the required information. Indeed, a long acquisition may represent a real waste of valuable instrument time. Second, the experiment time can often be reduced without any loss of resolution or sensitivity by judicious adjustment of the acquisition parameters shown in the next table. Here is a basic approach to obtaining acceptable COSY spectra in a reasonable time on the Gemini300:

1. Reduce nt to 8, or even 4, if possible. If you can obtain acceptable S/N in 256 scans or less in the 1D spectrum, nt=8 will work fine. If you can accept a higher level of baseline artifacts and have sufficient sample, you can use nt=4. Reducing nt from 16 to 8 will cut the experiment time in half. A 2 hr experiment is then a 1 hr experiment.

2. Reduce ni (number of 2d fids) to the lowest acceptable level (400-512 for very high resolution, 128-256 for medium to high resolution, 64-128 for low, but often adequate resolution). Reducing ni from 256 to 128 will cut the experiment time in half once again The 1 hr experiment is now only 30 min.

3. Reduce d1 to NO MORE THAN 1 to 1.5 times T1. If you are using D2O or DMSO-d6, relaxation can be quite short (0.2 to 0.5 sec) and a D1 of 0.3 to 0.6 may work quite well. Acetone-d6 or CD3OD may require larger d1 values (0.6 to 1.5 sec) for the best artifact reduction. Use the shortest possible d1. You can always redo the experiment if a quick 2D spectrum shows severe problems. You may decide at this point that the 400 or 500 might be needed to give better results. Even if you rerun the spectrum on the Gemini with a longer d1 value, you will have the information needed to make an appropriate choice. A short d1 can further reduce overall acquisition time by 25 to 50%.

4. ALWAYS, ALWAYS type time. Check to see how long the experiment will take before you proceed!


D. Summary

TO SUMMARIZE:

1) Acquire a 1d-proton spectrum and optimize the spectral width (movesw).

2) Move parameters to experiment 2, join experiment 2, and setup for the COSY pulse-sequence (mp(1,2), jexp2, cosy)

3) Adjust COSY parameters as needed to optimize time and resolution (adjust d1, nt, ni, and check time).


IV. Acquire the COSY Spectrum and Save it for Processing

At this point, simply acquire the COSY spectrum by typing go. WARNING: DO NOT TYPE ga. ga will acquire the spectrum and then immediately transforms each fid as they are acquired. This makes it impossible to transform the 2d spectrum on the fly.

After acquisition of the COSY spectrum is complete, save the data to disk by typing svf (or click Main Menu, and then 7:files on the menu bar). You can process and plot the 2D spectrum on the Gemini300 if no one is waiting. Otherwise, move to the workstations at this point. Remember, the use of the workstations frees up sorely needed time on the Gemini300 and makes possible acquisition of 2D spectra in our walk-up environment.


Acquire COSY       go                 go will clear the 2D space on the disk for the COSY  
                                      spectrum and will acquire the COSY                   

Save COSY          svf                svf (or Main Menu, 7:files) will save the COSY       
spectrum                              spectrum on the disk in a location that can be       
                                      easily accessed by the UNIX workstations.