# What does the $y$-axis represent in the atomic spectra and what is its significance?

The picture is an emission spectrum of Helium. The spectrum has sharp lines (peaks) at certain wave lengths characterizing it as helium. Agreed that it characterizes Helium as atomic spectral line characterize gases and they are based on allowed energy states of electrons in an atom.

Well and good, but what i don't know is the $y-axis$. what does it represent? It is shown as intensity (counts) but I want to know what it is and how does it vary from element to element. Does this count also characterize the elements, or is it same for all elements? Appreciate if you could throw some light on it.

Question : I mean if i keep the position of lines(pulses) same but change their relative amplitudes, what happens? does it represent a different gas?

Picture taken from the internet.

• This kind of figure is often called a "histogram" because it shows how many hits registered in a counter (making a proper histogram in the statistical sense), but the word is often used for plots of other measures of intensity as well. Aug 2, 2014 at 4:33

Here is the spectrum taken as a photo:

Note the difference in the visible intensity of the lines registered. In your spectrum instead of a film there is a counter which measures the number of hits at that wavelength from the excited helium.

The location of the excitations on the wavelength axis identifies the atom uniquely, like a fingerprint a person to the police. The intensity/counts is secondary to the identification, though it is characteristic it can depend on the intervening medium ( glass, air, space dust for astronomical observations).

• Does the relative amplitudes (not absolute) of the pulses in spectrum depend on the medium? Aug 2, 2014 at 4:09
• The detection can depend on the intervening medium, if it is more absorptive at some parts of the wavelength axis then the detection will change the ratio of intensities from the original emissions Aug 2, 2014 at 4:41
• Can we say theoretically in an ideal medium, or vaccum, the counts/amplitude should be same for all spectral peaks/lines ? Aug 2, 2014 at 5:20
• No. The strength on each line depends on the probability of that line being excited and the probability of falling back in and emitting a photon of distinct wavelength. For a given atom the strength is calculable for each line from the solutions of the equations that describe the orbitals of the electrons around the helium nucleus. It is different for each line. Though it is characteristic it is not as unaffected by the intervening medium and detector conditions as the location on the wavelength scale is. Aug 2, 2014 at 5:32
• In the figure, tgere are a dew small peaks which werent marked with wave length, assuming they arent considered as spectral lines, so is there any specific threshold on tge amplitude of peak for it to be considered as spectral line? Aug 2, 2014 at 6:00

It is what it claims to be: intensity of light at that wavelength.

However there are a lot of different ways to measure intensity. The "proper" way might be to measure the emitted power in watts into a particular wavelength bin, but that takes a lot of careful algebra and calibration to get right. If your light meter is a digitized CCD readout, however, it probably has an intensity measure for free that has been calibrated at the factory: each pixel on the CCD reports one1 number, where 0 means "no light struck this pixel" and some maximum number2 which means "this pixel received more light than it was able to record"). If you only care about those numbers along one dimension, you can make a plot of them instead of a two-dimensional image.

To show you how straightfoward it really is, here's the example spectrum from anna v's answer. I've taken a row of pixels near the middle of the image (row 60, actually, marked by the arrows) and plotted their red, green, and blue components on a graph. You can see that the blue lines have more blue than the other colors, that the red lines have more red than the other colors, and that the yellow line near pixel 160 is the brightest and is actually saturated (note the flat top and the artifact where the blue "shoulders" are dimmer than the background). You can imagine that I might get a more detailed spectrum graph if I just added up the numbers from all 120 rows of pixels in the image.

Other types of detectors may actually count photons one at a time, in which an axis that's labeled "counts" may actually mean "we counted this many photons in this wavelength bin." You have to read carefully to find what authors mean sometimes.

1 Actually a color CCD will report three numbers, one each for the red, blue, and green sensors nearest a given pixel. You can think of it as giving you three images with the same geometry.
2 If the analog-to-digital converter has $n$ bits of precision the maximum value is $2^n-1$. For 8-, 12-, 16-bit ADCs you get numbers between zero and 255, 4095, 16327.

As for the physics content of your question, each spectral line ideally has three parameters: a location, a height, and a width.

• The location of the lines tells you about the energy of the transition involved. Each species of atom has a particular set of energies that electrons are allowed to have, and therefore will have spectral lines whose wavelengths correspond to differences between these energies (as you've indicated that you already know).

• The intensity of each line (which is better represented by the area under each peak, rather than the height of the peak) tells you about how common a given transition is. Here is a tool that lets you examine and plot some solar spectral data; you'll see that the absorption lines for hydrogen and helium are very deep, while the absorption lines for other elements are much shallower. That tells you that most sun is made of hydrogen and helium.

• If you know that there is a relationship between some sets of spectral lines, you may be able to learn other information from their intensities. For instance the Lyman, Balmer, and Paschen series of hydrogen lines are due to light absorption by hydrogen atoms in their ground state, first excited state, and second excited state, respectively. If you find absorption lines in the Balmer or Paschen series, it means that the temperature of the hydrogen gas is so hot that some of the gas is getting excited from its ground state, then getting excited at least a second time before it has a chance to cool back down to the ground state. By (carefully) comparing the relative intensities of these related line series, you may be able to determine the temperature of the gas. This is how we know, for instance, that parts of the sun's corona are hotter than its photosphere.

• Finally each spectral "line" actually has some finite width. Part of that width is always intrinsic to the resolution of the spectrometer, but part is also due to thermal motion of the emitters and absorbers.

• "Actually a color CCD will report three numbers" — there is no such thing as a colour CCD. Rather to determine colour with CCDs, you put a colour filter in front of it. For a spectral analyser you wouldn't want to do that because the position already tells you everything about the frequency, so any filter would not add any information. Aug 2, 2014 at 18:50
• @celtschk Since my example spectrum was taken from a color photo I thought it was worthwhile to mention what was happening there. Excellent point, though.
– rob
Aug 2, 2014 at 19:58