OPERA experiment - Special Relativity

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Homework Help Overview

The problem involves the OPERA experiment, which reported neutrinos appearing to travel faster than light, raising questions about their mass and energy. The discussion centers around the equations relating energy, momentum, and mass in the context of special relativity.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between energy, momentum, and mass, questioning the implications of differentiating the energy-momentum equation. Some express confusion about the meaning of the derivative ##\frac{\delta E}{\delta p}## and its application. Others discuss the implications of mass for particles traveling at or above the speed of light.

Discussion Status

The discussion is ongoing, with participants sharing various approaches to the problem. Some have provided hints and suggestions for differentiation, while others express uncertainty about their calculations and the underlying concepts. There is no explicit consensus on the correct approach or interpretation of the results.

Contextual Notes

Participants note the historical context of the OPERA experiment and its eventual conclusion regarding measurement errors. There is also mention of the implications of mass for particles traveling faster than light, which adds complexity to the problem.

Isaac Pepper
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Homework Statement


In 2011, researchers at the OPERA experiment thought they had seen neutrinos with mass m and energy E = 28 GeV moving faster than light. The baseline between the source and the detector was 731 km, and the neutrinos seemed to arrive 60.7 ns early, compared to the maximum physical velocity c. (a) Using ##m^2c^4 = E^2 - p^2c^2 ##with p the momentum of the neutrinos, show that ##v = \frac{\delta E}{\delta p}= c\sqrt{1-\frac{m^2c^4}{E^2}}##. (b) Calculate the mass of such faster-than-light neutrinos in ##GeV/c^2##

Homework Equations


##p=\gamma mv##
##m^2c^4=E^2-p^2c^2##

The Attempt at a Solution


(a) ##m^2c^4=E^2-p^2c^2##
I've tried many calculations and never managed to find the correct result. I don't really understand the ##\frac{\delta E}{\delta p}##.
Am I right in trying to convert ##p## to ##mv## or is it ##p=\gamma mc##?
By using ##p=mv##, I manage to get :
$$m^2c^4=E^2-m^2v^2c^2$$
$$\frac{E^2-m^2c^4}{m^2c^2}=v^2$$
$$\frac{E^2}{m^2c^2}-c^2=v^2$$
$$v^2=c^2(\frac{E^2}{m^2c^2}-1)$$
$$v=c\sqrt{\frac{E^2}{m^2c^4}-1}$$
But this isn't using ##\frac{\delta E}{\delta p}## and the result isn't quite right. What am I missing?

(b) I'm kind of fuzzy on this - to me, photons traveling at the speed of light are massless, and if I apply the given formula to find the mass of a neutrino traveling faster than light...Well I hit a dead-end because it would be less than massless? Atleast that's the way I see it.
I've managed to work out the speed of the neutrino if it arrives 60.7ns earlier than light, which would be ##v=300007473 m.s^{-1}## assuming that ##c=3.0*10^8 m.s^{-1}##
All calculations including a gamma factor would not work to me, as ##1-\frac{v^2}{c^2}## would be less than 0
so the square root in the gamma factor would be less than 0... How would I then calculate the mass of the faster-than-light neutrino?

Thanks to everyone for the amazing help!
 
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Any help would be greatly appreciated, I'm still stuck on the question. Sorry for the double post.
 
Hi there Issac
Isaac Pepper said:
How would I then calculate the mass of the faster-than-light neutrino?

you did understand that the experiment gave the incorrect answer because of equipment failure ?

and NOTHING with mass can travel at c, let alone fasterDave
 
davenn said:
you did understand that the experiment gave the incorrect answer because of equipment failure ?

and NOTHING with mass can travel at c, let alone faster
Dave

I do understand that, which is partly why I don't understand what the question is asking me...
Any ideas on how to solve this? I don't even understand how to do part (a) at this point
 
Isaac Pepper said:

Homework Statement


In 2011, researchers at the OPERA experiment thought they had seen neutrinos with mass m and energy E = 28 GeV moving faster than light. The baseline between the source and the detector was 731 km, and the neutrinos seemed to arrive 60.7 ns early, compared to the maximum physical velocity c. (a) Using ##m^2c^4 = E^2 - p^2c^2 ##with p the momentum of the neutrinos, show that ##v = \frac{\delta E}{\delta p}= c\sqrt{1-\frac{m^2c^4}{E^2}}##. (b) Calculate the mass of such faster-than-light neutrinos in ##GeV/c^2##

For part a), why not start by differentiating (wrt ##p##):

##E^2 = p^2c^2 + m^2c^4##

PS For b) Part a) gives you an equation for mass without the ##\gamma## factor. So, you could calculate an imaginary mass.
 
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PeroK said:
For part a), why not start by differentiating (wrt ##p##):

##E^2 = p^2c^2 + m^2c^4##

Ok, even then I'm not sure how to differentiate this expression with respect to p
I can re-arrange to get ##E=\sqrt{m^2c^2+p^2c^2}## but I don't know how to differentiate that wrt p
 
Isaac Pepper said:
Ok, even then I'm not sure how to differentiate this expression with respect to p
I can re-arrange to get ##E=\sqrt{m^2c^2+p^2c^2}## but I don't know how to differentiate that wrt p

Perhaps time to revise differentiation? It's easier, in any case, to leave it as ##E^2## and differentiate implicitly (if that's something you know how to do).
 
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PeroK said:
Perhaps time to revise differentiation? It's easier, in any case, to leave it as ##E^2## and differentiate implicitly (if that's something you know how to do).
Have you calculated it? I'm curious whether my 9.756 i MeV are correct?
 
fresh_42 said:
Have you calculated it? I'm curious whether my 9.756 i MeV are correct?
Do you mean for part (b) ?

I have done $$v=c\sqrt{1-\frac{m^2c^4}{E^2}}$$
$$v^2=c^2-\frac{m^2c^6}{E^2}$$
$$m^2=\frac{E^2(c^2-v^2)}{c^6}$$
$$m=\frac{1}{c^2}\sqrt{E^2-\frac{E^2v^2}{c^2}}$$
Plugged in numbers and got : $$m=\frac{28}{(3*10^8)^2}i\sqrt{4.98*10^{-5}}=\frac{28}{(3*10^8)^2}i*7.06*10^{-3} GeV/c^2$$
It's probably wrong at this point, I'm totally lost and have given up on (a) :/
 
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  • #10
I'm not sure whether my calculation is correct. I kept ##c## as long as possible, set ##c + ε = \frac{d}{1-t}## with ##d = 1## lightsecond and ##t=60.7 ns##. Then I broke all down to ##m = 28 GeV \cdot c^{-1} \cdot \sqrt{-2cε - ε^2} ## from the solution in (a) and substituted ##ε## by ##t## until I got a factor ##\sqrt{ 1- \frac{1}{(1-t)^2}}##. I didn't start with actual numbers not until this term. But there have been so many rearrangements that I'm not sure anymore.

I solved part (a) with PeroK 's hint. ## \frac{∂}{∂p} E^2 = 2 E\cdot \frac{∂}{∂p}E = \frac{∂}{∂p}(m^2 c^4) + \frac{∂}{∂p} (p^2c^2) = 0 + 2pc^2 ## and ##pc^2 E^{-1} = c \sqrt{1- \frac{m^2 c^4}{E^2} }## is just another expression for ##E^2 = m^2 c^4 + p^2 c^2##.

EDIT: My ##GeV## are actually ##GeV / c^2##. How did you get ##v##?
 
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  • #11
fresh_42 said:
How did you get ##v##?

If the neutrino arrived ##60.7*10^{-9}s## before light would, then ##t_2-t_1=\frac{d}{v}-\frac{d}{c}=-60.7*10^{-9}s##
In which case ##t_2-t_1+\frac{d}{c}=\frac{d}{v}##
$$v=\frac{d}{t_2-t_1+\frac{d}{c}}=\frac{731*10^3}{-60.7*10^{-9}+\frac{731*10^3}{3*10^8}} = 300 007 473.5 m.s^{-1}$$
Atleast that's what I thought!

EDIT : I follow your implicit differentiation, but how do you end up with ##pc^2E^{-1} = c\sqrt{1-\frac{m^2c^4}{E^2}}## ?
 
  • #12
Yep, that's my calculation of ##v = \frac{d}{1-t}##, too (since ##d/c## is numerically just ##1##).

##\frac{p^2c^2}{E^2} = \frac{E^2 - m^2 c^4}{E^2} = 1 - \frac{m^2c^4}{E^2} ⇒ \frac{pc}{E} = \sqrt{1 - \frac{m^2 c^4}{E^2}} ⇒ \frac{pc^2}{E} = c \cdot \sqrt{1 - \frac{m^2 c^4}{E^2}}##
 
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  • #13
Fair enough, I know the calculations I did after it were wrong though, so ignore them, I'm sure you have the right answer ! I will look through what I have done in the morning to try and work it out. Thank you for all your help, both of you !
 
  • #14
Isaac Pepper said:
$$m=\frac{1}{c^2}\sqrt{E^2-\frac{E^2v^2}{c^2}}$$
Until here we are identically. Pulling ##E^2## out of the root gives us ## m = 28GeV \cdot \sqrt{1 - \frac{v^2}{c^2}}##

Plugged in numbers and got : $$m=\frac{28}{(3*10^8)^2}i\sqrt{4.98*10^{-5}}=i*7.06*10^{-3} GeV/c^2$$
It's probably wrong at this point, I'm totally lost and have given up on (a) :
Sorry for you, you are not wrong. I am. ##\frac{c}{v} = 1-\frac{c}{d}Δt ## where ##d=731,000 m ## and ##Δt = 60.7 ns##.
(I calculated ##\frac{c}{v} = 1-Δt## which is the wrong velocity.)

Your correct result is ##\frac{v}{c} = 1+ 2.4912 * 10^{-5}##
Therefore ##m = 28 GeV \cdot \sqrt{1 - (1 + 2.4912 * 10^{-5} )^2} = 28 GeV \cdot 7.06 \cdot 10^{-3}i = 197.68 i MeV##

EDIT: If ##28 GeV## is already divided by ##c^2## as usual. Forgot some i.
 
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  • #15
Yeah, that seems to my solution too, though I divided it by ##c^2## so my answer was $$\frac{28GeV}{(3*10^8)^2}*i*7.06*10^{-3}=i*2.20*10^{-18} GeV/c^2$$
 
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  • #16
Isaac Pepper said:
Yeah, that seems to my solution too, though I divided it by ##c^2## so my answer was $$\frac{28GeV}{(3*10^8)^2}*i*7.06*10^{-3}=i*2.20*10^{-18} GeV/c^2$$
A like this kind of poorness: two footsore guys made it together over the goal line ...:wink:
 
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