In order to enable an iCal export link, your account needs to have an API key created. This key enables other applications to access data from within Indico even when you are neither using nor logged into the Indico system yourself with the link provided. Once created, you can manage your key at any time by going to 'My Profile' and looking under the tab entitled 'HTTP API'. Further information about HTTP API keys can be found in the Indico documentation.
Additionally to having an API key associated with your account, exporting private event information requires the usage of a persistent signature. This enables API URLs which do not expire after a few minutes so while the setting is active, anyone in possession of the link provided can access the information. Due to this, it is extremely important that you keep these links private and for your use only. If you think someone else may have acquired access to a link using this key in the future, you must immediately create a new key pair on the 'My Profile' page under the 'HTTP API' and update the iCalendar links afterwards.
Permanent link for public information only:
Permanent link for all public and protected information:
We analysed from a bottom-up approach the level of tuning in the MSSM and in the NMSSM associated with the measured 126 GeV Higgs mass, direct searches of superpartners and collider measurements of the Higgs couplings to fermions and gauge bosons. In particular we show that in the scale invariant NMSSM, TeV-scale stop masses are still allowed in much of the parameter space with 5 $\%$ tuning for a low messenger scale, split families and a Higgs-singlet coupling $\lambda$ of order one. In the absence of deviations of the Higgs couplings to fermions and massive gauge bosons from SM values at the LHC and in future colliders, we noticed that there is an additional independent tuning due to the "SM-likeness" requirement, which can be naturally suppressed in the MSSM for large values of $\tan\beta$ but that in the scale invariant NMSSM for a coupling $\lambda$ of order one can be the dominant source of tuning.