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Javascript move mouse to other element on mouse over

Hi and thanks in advance!
I have a dropdown menu with a sidebar on the left. I also have a button which if clicked should highlight the button and move the mouse to the arrow that points to the button. How do I achieve this?
I use this to point to the arrow, but how do I change it to move the mouse?

‘Foo’

A:

function toggleSidebar() {
if (document.body.style.display == ‘block’) {
document.body.style.display = ‘none';
} else {
document.body.style.display = ‘block';
}
}
Mouse Over

document.body is the body of the page. If we use this value in our example, we can move the cursor to the header of the page.
It’s just as simple as saying in our CSS that the body is a selector and we can change it’s style in JavaScript.

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All comments are moderated. The Council is not responsible for the content of the comments. All views expressed are those of the commenter and may not necessarily represent the views of the Council or its members unless specifically.-2}$ $9\times10^{ -2}$
————————————– ————————————- ————————————-

: Best fit parameters to the data, for various types of contamination.[]{data-label= »tab:fits »}

The main result of this study is the absence of contamination, which we can firmly rule out with a $3\sigma$ confidence. This null result can be used to improve the bounds on sterile neutrino mixing from reactor neutrino experiments, by rejecting the possibility that the oscillation anomaly is caused by residual contamination of the detectors.

If a sterile neutrino is indeed present, there will be new physics in the neutrino sector: the sterile neutrino will be heavier than any Standard Model fermion, and therefore it will not be affected by the high energy LHC physics. Its mixing with neutrinos will depend on the mechanism responsible for neutrino mass generation: the sterile neutrino mass will be below 10 GeV for Dirac mass (case A) and below $10^{7}~{\rm GeV}$ for Majorana mass (case B). The mixing with Standard Model neutrinos will also depend on this mass, through the mixing angle $\theta$, which can be large for case A and negligible for case B.

The dependence of the sterile neutrino mixing on the neutrino mass is not the only discovery potential. In the case of Majorana mass the sterile neutrino will naturally have a large magnetic moment. To be more precise, it will possess a non-zero magnetic dipole moment along the direction of the magnetic field. This can be tested by searching for the energy shift induced in $\beta$-decay due to the spin of the nucleus and the neutrino: the calculated value of this shift, ${\cal
O}(10^{ -2})~\mu_{\rm B}$, is comparable to the accuracy of current measurements. As an example, for the A2 experiment, the expected shift in a $2~{\rm g/l}$ CdWO$_4$ detector is $\delta E_{\beta}=0.03\cdot
E_{\beta}\