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benzun_1999 Nov19-03 05:18 AM

Quantum number.
 
hi all,

What is quantum number????????[:D]

I know a bit about quantum number but i am not clear about it so can anyone please help me?. [t)]

-Benzun,
All for God.

jcsd Nov19-03 07:57 AM

When a property of a system can only take certain discrete values each discrete value that property has a quantum number whose value is detimned by which discrete state it is in, for example the angular momentum of an electron in a bound state of an atom can only take values of nh/2&pi, where n is and integer and is the quantum number.

lethe Nov19-03 10:43 AM

a quantum number is an eigenvalue of an observable from some maximally commuting set of observables of your system.

quantum numbers include, n for energy level, spin, mass, charge. and more...

i would not say that a quantum number must only take discrete values, although this is usually the case.

benzun_1999 Nov20-03 06:01 AM

could you please explain a bit more(use,properties,formula,etc)

drag Nov20-03 01:20 PM

Greetings !

Try this and follow the other links:
http://hyperphysics.phy-astr.gsu.edu.../qunoh.html#c2

Peace and long life.

lethe Nov21-03 07:03 AM

every time the system has a symmetry, there is a quantum number that labels which state of the symmetry that the system is in.

for example, there are many ways that rotations can act on a quantum system, and if the system is a rotationally symmetric one, then whenever the system starts in one of those states, it has to remain that state.

the spin quantum number is just a number to label which of those states the system is in.

Luquido Lumino Nov28-03 02:24 AM

Single unit differentiation
 
A quantum number as far as I can recognize is the single unit value in a non abstractive measure therefore if the number 3 has a value in a Chronograph it would be subject relative to its effect of angular definition.

I am still only a student so I may be wrong.

mormonator_rm Dec1-03 10:22 AM

Quantum numbers
 
There are a whole lot of quantum numbers associated with different fields and particles. Its all about quantization; various properties can only be had in certain discreet values. The quantum numbers are actually just a description of how many of these discreet units are present in a given object.

For example, I deal alot with mesons (particles that consist of a quark and an antiquark in a bound system), and there are a number of quantum numbers to deal with. First of all, there are quantum numbers for angular momentum and spin momentum, called l and s respectively. There are also flavor quantum numbers, including isospin (I), strangeness (S), charm (C), bottom (B) and top (T). The isospin is a property of the lightest quarks (up and down), while the others are properties of the heavier quarks. There is also the baryon number (b). All quarks have an intrinsic baryon number of 1/3 and their antiquarks have baryon number -1/3. The result is that baryons have b = 1 and mesons have b = 0 (which is the natural result, after all).

The l and s quantum numbers can be combined through a process called "coupling", which is like addition;

j = l '+' s
= {[l+s], [l+s-1],..., [l-s]}

but it allows all the values in between the addition and subtraction of the two, as shown above. The result of coupling is the total momentum number j.

There are also quantum numbers associated with symmetries here. There is a parity number P which is either +1 or -1 based on the equation;

P = (-1)^l+1

a charge conjugation number based on the formula;

C = (-1)^l+s

and a G-parity number based on the formula;

G = (-1)^l+s+I

which includes the isospin in the symmetry. There is also a radial excitation quantum number N that is useful.

When we represent the quantum states that are occupied by mesons, we generally form the multiplets of mesons based on the quantum numbers N, l, s, j, P, and C. Within these multiplets are members with different values of I, G, S, C, B and T numbers as well. All mesons have b = 0. So we generally represent the mesons, in written form, by the statement IG(JPC). For example, the pion can be represented as 1-(0-+), the eta meson as 0+(0-+), the kaon as 1/2(0-). They all occur in the same multiplet, the ground state pseudoscalar multiplet with (0-+) being the key defining numbers there. *The kaon is a spin 1/2 particle, and hence not an eigenstate of C, thus the C and G numbers are ommited.

So there's some examples of how quantum numbers are used to keep track of which particles are which and how they are related to each other.


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