Why can't neutrinos be brought to rest?

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Neutrinos, despite having mass, cannot be brought to rest due to their extremely weak interactions with matter, primarily through the weak force and gravity. Unlike other massive particles, which can be confined using electromagnetic forces, neutrinos rarely interact, making them difficult to capture. The discussion also touches on the behavior of neutrinos during processes like beta decay and in environments such as supernovae, where high matter density may temporarily confine them. Additionally, the Heisenberg Uncertainty Principle complicates the idea of bringing any particle, including neutrinos, to a complete rest state. Ultimately, while theoretically possible under certain extreme conditions, practically capturing and slowing neutrinos remains nearly impossible.
  • #31
nikkkom said:
Easy peazy.
Observe a stationary tritium atom's decay. Measure electron's impulse and calculate neutrino's impulse, then jump into your standard-issue near-lightspeed spacecraft and catch up to the neutrino.
Bingo. You have it stationary in your frame of reference.

Wonderful! My dream has come true! Please build me one! I need it next week.

Zz.
 
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  • #32
anorlunda said:
Low speed neutrinos might be more likely to interact with ordinary matter. By analogy, fast neutrons in a reactor are slowed to thermal speed to find the resonance peaks at lower neutron energies where fission events are much more likely. I presume that the physics of slow speed neutrinos have never been studied because there was no reason to do so.

Actually, the opposite is the case. The lower the neutrino energy, the lower the interaction cross section. A neutrino with a few ev (still moving > .99c) has such a low interaction cross section that even neutron star core is effectively transparent to it. A neutron star provides a thought experiment for slowing neutrinos: for high energy neutrinos, the mean free path is small compared to neutron star radius. However, as neutrinos slow to a .99c, they all escape.

Two of the scenarios proposed so far do seem to work for producing neutrinos slow compared to c:

- primordial big bang neutrinos
- black hole event horizons Hawking radiation (some will be slow neutrinos)

However, the insanely low interaction cross section means we will never detect these. If a neutron star core is transparent to these, what hope have we?
 
  • #33
Suppose I gave you a fist full of thermal (ie, slow) neutrinos. How would you know?
 
  • #34
.Scott said:
Suppose I gave you a fist full of thermal (ie, slow) neutrinos. How would you know?

Exactly, you couldn't know. You would never be able to distinguish it from a fist full of nothing.
 
  • #35
I would ask you to release them close to PTOLEMY, once it is build.
They aim to measure relic neutrinos from the big bang, together with a direct mass measurement.
 
  • #36
What a great provocative question Scott.

If neutrinos were stationary so that they could be located within a nucleus or within a hadron, for an indefinite period of time, then I guessed that interactions might be much more likely. I know that interactions between free neutrons and nuclei are hugely dependent on relative velocities, why should neutrinos be different?

Since we have never seen slow neutrinos, I presume that experimental physics has no data on the interaction properties of slow neutrinos. That is why I intended my original post to be directed at theoretical physics rather than experimental physics. Photons must move at velocity c. Fermions must obey the Pauli exclusion principle. Those properties can be derived from the wave functions. I am curious to learn if there are analogous theoretical principles for neutrinos that dictate their peculiar properties.
 
  • #37
Neutrinos are fermions. They have well-predicted (by the standard model) interactions with matter, and if they are slow their interaction cross-section is low.
 
  • #38
mfb said:
Neutrinos are fermions. They have well-predicted (by the standard model) interactions with matter, and if they are slow their interaction cross-section is low.

If we can't detect slow vs. fast neutrinos, then how can we tell how much of the neutrino's energy is rest mass and how much is due to velocity?
 
  • #39
There are upper limits on the mass. Sure, the cross-section at low energies will depend on the (still unknown) mass, but as far as I know it will be small for all possible masses.
 
  • #40
Chase it!

anorlunda said:
If neutrinos were massless, they would have to travel at c. But now we know they have mass, so they must travel at speeds less than c.

But (all?) other massive particles can be brought to rest. Why not neutrinos? Is there a theoretical reason that forbids it?

Climb into your vehicle of choice and accelerate in pursuit of the (massive) neutrino - when you catch up with it, slow down and move alongside it. Now it is at rest w.r.t. you, and you didn't even have to touch it :) [although General Relativity tells us that you could interpret what happened as the appearance of a gravitational field in your frame of reference, which brought the neutrino to rest beside you: you avoided falling by using your vehicle's power-thrusters].

Easier said than done, of course.
 
  • #41
We would need an experimental setup capable of isolating a single neutrino - which would be an impressive accomplishment. It's relatively easy to isolate an electron.
 
  • #42
OK, I think I understand now thanks to your help. Let's see if I got it right.

The original question could have been phrased as a paradox. If neutrinos are massive, why don't we see a spectrum of non-relativistic velocities for them as we do for other massive particles? Wikipedia says that the lower limit for neutrino velocities is 0.999976 c.

The apparent answer requires two logical steps.

First, when neutrinos are emitted:

(mfb put numbers on it, and that helped me to understand.)

mfb said:
... A .23eV-neutrino with a kinetic energy of .10 meV moves with ~9000km/s ...

So for the sake of argument let's say that when emitted, neutrinos have a wide distribution of energy in excess of rest mass. But because the rest mass is so small, only a tiny kinetic energy is needed for relativistic speeds. Therefore, the fraction of all energies corresponding to non-relativistic speeds is tiny.

Second, after emission: Because neutrinos interact so little with other particles, they do not become thermalized. They tend to conserve whatever energy they were emitted with.

Put those two things together and we can see that it is possible to have neutrinos at any speed 0<v<c. However, non-relativistic speeds are very improbable.

The seeming paradox comes from confusing what's possible with what's probable. Secondary confusion comes from using the word possible in the ideal sense, contrasted with possible pragmatically in the laboratory.
 
  • #43
anorlunda said:
Wikipedia says that the lower limit for neutrino velocities is 0.999976 c.
For a specific energy (here: 3 GeV). Hmm, that part of the article is outdated.

So for the sake of argument let's say that when emitted, neutrinos have a wide distribution of energy in excess of rest mass. But because the rest mass is so small, only a tiny kinetic energy is needed for relativistic speeds. Therefore, the fraction of all energies corresponding to non-relativistic speeds is tiny.
Right.

Second, after emission: Because neutrinos interact so little with other particles, they do not become thermalized. They tend to conserve whatever energy they were emitted with.
Right.

Put those two things together and we can see that it is possible to have neutrinos at any speed 0<v<c. However, non-relativistic speeds are very improbable.
Right.
 
  • #44
What is the shape of the tail of the beta decay?
If 100 % of the antineutrinos emitted by tritons have energy under 18 keV (because that is the total energy of the beta decay), what percentage have energy under 1800 eV? 180 eV? 18 eV et cetera?
 
  • #45
There is a formula for the electron energy spectrum. The neutrino energy is the difference between the total energy and the electron energy.

Close to the endpoint (and neglecting the neutrino mass), the probability is quadratic with the difference to that endpoint. The fraction of neutrinos below 1800 eV is roughly 1% (guessed, should be right up to a factor of ~5), the fraction below 180 eV is roughly 0.001% and so on - every factor of 10 reduces the fraction of neutrinos by a factor of 1000.
 
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