Recent null results from LHC8 SUSY searches along with the discovery of a
SM-like Higgs boson with mass m(h) ~ 125.5 GeV indicates sparticle masses in
the TeV range, causing tension with conventional measures of electroweak
fine-tuning. We propose a simple Fine-tuning Rule which should be followed
under any credible evaluation of fine-tuning. We believe that overestimates of
electroweak fine-tuning by conventional measures all arise from violations of
this rule. We show that to gain accord with the Fine-tuning Rule, then both
Higgs mass and the traditional \Delta_{BG} fine-tuning measures reduce to the
model-independent electroweak fine-tuning measure \Delta_{EW}. This occurs by
combining dependent contributions to m(Z) or m(h) into independent units. Then,
using \Delta_{EW}, we evaluate EW fine-tuning for a variety of SUSY models
including mSUGRA, NUHM1, NUHM2, mGMSB, mAMSB, hyper-charged AMSB and nine cases
of mixed moduli-anomaly (mirage) mediated SUSY breaking models (MMAMSB) whilst
respecting LHC Higgs mass and B-decay constraints (we do not impose LHC8
sparticle mass constraints due to the possibility of compressed spectra within
many of these models). We find mSUGRA, mGMSB, mAMSB and MMAMSB models all to be
highly fine-tuned. The NUHM1 model is moderately fine-tuned while NUHM2 which
allows for radiatively-driven naturalness (RNS) allows for fine-tuning at a
meager 10% level in the case where m(higgsinos) ~ 100-200 GeV and the TeV-scale
top squarks are well-mixed. Models with RNS may or may not be detect at LHC14.
A \sqrt{s} ~ 500 GeV e^+e^- collider will be required to make a definitive
search for the requisite light higgsinos.Comment: 30 pages and 12 figures; revised version includes additional
references and several typo fixe