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Thermonicolet Omnic Software User's Guide 6.1 (PDF) - Charles E ...

Thermonicolet Omnic Software User's Guide 6.1 (PDF) - Charles E ...

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Only one spectrum can be displayed in a pane. Stacking spectra is useful when<br />

you are comparing spectra that are significantly different. For example, stacking<br />

the library spectra found in a spectral search can make it easier to decide which<br />

spectrum most closely matches the unknown sample.<br />

When you stack spectra, you set the number of panes in the spectral window by<br />

using Display Setup in the View menu (see “Specifying how to stack spectra” in<br />

the “View” chapter for details). There can be more panes in the window than there<br />

are spectra, resulting in one or more empty panes. There can also be more spectra<br />

in the window than there are panes. In this case some spectra may be out of view<br />

“above” or “below” the panes. You can scroll spectra into view or into an empty<br />

pane (this is explained below).<br />

Each pane in the stack has its own Y-axis. Any X-axis adjustments that you make<br />

using the view finder will affect all of the spectra in the window.<br />

Displaying a list of stacked spectra – Click the arrow at the right end of the<br />

title box to see a list of all the spectra in the window, including those out of view.<br />

The spectrum titles appear in the list in order from top to bottom.<br />

Hiding a stacked spectrum – Use Hide Spectra in the View menu to hide a<br />

stacked spectrum so that it doesn’t appear on the screen (see “Hiding spectra” in the<br />

“View” chapter for details). When a stacked spectrum is hidden, its title appears in<br />

the font specified for the titles of hidden spectra in the View options. The default<br />

font for displaying the titles of hidden spectra is italic. (See “Specifying fonts for<br />

displayed text” in the “Edit” chapter.) In the example below, the spectrum titled<br />

“Aromatic Compound” is hidden.<br />

OMNIC User’s <strong>Guide</strong> 41

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