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As explained in this article, as the CMB is created from a vaiable (matter?) density $\kappa$ its gradient $\nabla \kappa = \vec{u}$ can be separated into a gradient and curl part, called the $E$ and $B$ modes

$$ \nabla^2 \kappa^E = \nabla \cdot \vec{u} $$

and

$$ \nabla^2 \kappa^B = \nabla \times \vec{u} $$

Thinking about electromagnetism, these definitions look slightly (but not exactly) familiar, if the vector $\vec{u}$ would take the role of the electromagnetic potential $\vec{A}$.

Is the similarity to the terminology of electromagnetism just a coincidence, or do these $E$ and $B$ modes have indeed something to do with electric and magnetic fields ?

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Could you refer to the article where the equations come from? Usually $E$ and $B$ vectors design the electric and magnetic field, respectively. –  Py-ser Mar 16 at 3:50
    
It is not a coincidence; it reflects that one of the component is curl free and the other not. But it does not refer to any electro- magnetic field. –  chris Mar 16 at 15:32
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In this context, the $\kappa$ you are referring to is called the dimensionless matter density field. It is gravitational lensing jargon, and is usually just referred to as the 'convergence' field.

What you have written there (that a field can be split up into divergence-less and curl-less components) is generally speaking true for any field which can be expressed as the curl of another field $A$. @chris is correct in that they refer not to the electromagnetism you are probably used to hearing these types of things discussed in, but refer to the polarization states of the cosmic microwave background due to quantum fluctuations in the early universe. They are called 'E' and 'B' only because they are reminiscent of electric and magnetic field lines.

The big find was the measurement of B-modes. As a reminder, here is what these E- and B-mode patterns in the CMB would look like: enter image description here

The big thing here is that E-modes are symmetric upon reflection, whereas B-modes are clearly not ($B>0$ maps into $B<0$). In order to produce B-mode polarization, you need two things:

1) Thompson scattering of photons by free electrons (present in the surface of last scattering as well as reionization).

2) A temperature quadrupole.

The exciting thing about the second item is that there are only a few things which can produce just such a quadrupole moment, and one of them is gravity waves! Gravitational waves physically warp the coordinates of space-time as it travels through space, which of course have existing particles, causing these types of distortions:

gravmode1gravmode2

This is the source of the temperature quadrupole moments. Sides which are squeezed are hotter and sides which are stretched are cooler.

Gravitational lensing can also produce small amounts of B-mode like features in the cmb polarization, but I believe they occur on much smaller scales and can therefore be ruled out as the cause of the BICEP2 findings. Lensing tends to stretch things out perpendicular to the radial vector (in the $\hat{\theta}$ direction): weaklensing

The reason why this matters is because lensing provides a mechanism for turning E-mode polarization (take the $E<0$ mode for example) into a B-mode type polarization. Most plots of the BICEP2 results show the effect of lensing at much higher multipole moment (i.e. - smaller physical scales), so I believe they have a good way of differentiating between the two types of secondary cmb anisotropies.

bicep2

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Thanks for this nice answer and claritication, I have already seen such a picture for example from the press announcement :-). What always looks slightly strange to me is, that it seems that in the pattern for $E>0$ it looks from a naive point of view that if the lines are $\vec{u}$ then $\nabla\vec{u} = 0$ than positive ... Can you give more details about how gravitational waves can produce temperature quadrupoles and generally about the mechanism 2 ? –  Dilaton Mar 23 at 21:59
    
OK - the details are added. Let me know if any further clarification is needed. –  astromax Mar 24 at 15:02
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