Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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4140 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{7}q_{1}q_{2}$ + ${ }M_{2}M_{8}$ | 0.6886 | 0.8712 | 0.7903 | [M:[0.9986, 1.0774, 1.1533, 0.8467, 0.692, 1.0014, 0.692, 0.9226], q:[0.7693, 0.5387], qb:[0.4627, 0.384], phi:[0.4613]] | [M:[[13], [-4], [5], [-5], [3], [-13], [3], [4]], q:[[-1], [-2]], qb:[[-11], [6]], phi:[[2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{5}$, ${ }M_{7}$, ${ }M_{4}$, ${ }M_{8}$, ${ }\phi_{1}^{2}$, ${ }M_{6}$, ${ }M_{3}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}M_{5}$, ${ }M_{4}M_{7}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{4}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{4}M_{8}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{3}M_{7}$, ${ }M_{8}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{4}M_{6}$, ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{7}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{6}M_{8}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{1}$, ${ }M_{7}q_{1}\tilde{q}_{1}$ | ${}$ | -2 | 2*t^2.076 + t^2.54 + 2*t^2.768 + t^3.004 + t^3.46 + t^3.688 + t^3.696 + 4*t^4.152 + t^4.16 + t^4.388 + 3*t^4.616 + 4*t^4.844 + 3*t^5.08 + 2*t^5.308 + 4*t^5.536 + t^5.544 + t^5.764 + 3*t^5.772 - 2*t^6. + t^6.008 + 7*t^6.228 + 2*t^6.236 + 2*t^6.456 + 2*t^6.464 + 4*t^6.692 + 2*t^6.7 + 6*t^6.92 + 2*t^6.928 + 6*t^7.156 + t^7.164 + t^7.376 + 3*t^7.384 + t^7.392 + 6*t^7.612 + 2*t^7.62 + 2*t^7.84 + 5*t^7.848 + t^7.856 - 3*t^8.076 + 3*t^8.084 + 12*t^8.304 + 3*t^8.312 + t^8.321 + 2*t^8.532 + 2*t^8.548 + t^8.768 + 6*t^8.776 + 9*t^8.996 - t^4.384/y - (2*t^6.46)/y + (3*t^7.616)/y + (4*t^7.844)/y + (2*t^8.08)/y + (4*t^8.308)/y + t^8.544/y + (2*t^8.764)/y + (4*t^8.772)/y - t^4.384*y - 2*t^6.46*y + 3*t^7.616*y + 4*t^7.844*y + 2*t^8.08*y + 4*t^8.308*y + t^8.544*y + 2*t^8.764*y + 4*t^8.772*y | 2*g1^3*t^2.076 + t^2.54/g1^5 + 2*g1^4*t^2.768 + t^3.004/g1^13 + g1^5*t^3.46 + g1^14*t^3.688 + t^3.696/g1^12 + 4*g1^6*t^4.152 + t^4.16/g1^20 + t^4.388/g1^11 + (3*t^4.616)/g1^2 + 4*g1^7*t^4.844 + (3*t^5.08)/g1^10 + (2*t^5.308)/g1 + 4*g1^8*t^5.536 + t^5.544/g1^18 + g1^17*t^5.764 + (3*t^5.772)/g1^9 - 2*t^6. + t^6.008/g1^26 + 7*g1^9*t^6.228 + (2*t^6.236)/g1^17 + 2*g1^18*t^6.456 + (2*t^6.464)/g1^8 + 4*g1*t^6.692 + (2*t^6.7)/g1^25 + 6*g1^10*t^6.92 + (2*t^6.928)/g1^16 + (6*t^7.156)/g1^7 + t^7.164/g1^33 + g1^28*t^7.376 + 3*g1^2*t^7.384 + t^7.392/g1^24 + 6*g1^11*t^7.612 + (2*t^7.62)/g1^15 + 2*g1^20*t^7.84 + (5*t^7.848)/g1^6 + t^7.856/g1^32 - 3*g1^3*t^8.076 + (3*t^8.084)/g1^23 + 12*g1^12*t^8.304 + (3*t^8.312)/g1^14 + t^8.321/g1^40 + 2*g1^21*t^8.532 + (2*t^8.548)/g1^31 + g1^4*t^8.768 + (6*t^8.776)/g1^22 + 9*g1^13*t^8.996 - (g1^2*t^4.384)/y - (2*g1^5*t^6.46)/y + (3*t^7.616)/(g1^2*y) + (4*g1^7*t^7.844)/y + (2*t^8.08)/(g1^10*y) + (4*t^8.308)/(g1*y) + t^8.544/(g1^18*y) + (2*g1^17*t^8.764)/y + (4*t^8.772)/(g1^9*y) - g1^2*t^4.384*y - 2*g1^5*t^6.46*y + (3*t^7.616*y)/g1^2 + 4*g1^7*t^7.844*y + (2*t^8.08*y)/g1^10 + (4*t^8.308*y)/g1 + (t^8.544*y)/g1^18 + 2*g1^17*t^8.764*y + (4*t^8.772*y)/g1^9 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
2165 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{7}q_{1}q_{2}$ | 0.6816 | 0.86 | 0.7926 | [M:[1.013, 1.0729, 1.1588, 0.8412, 0.6953, 0.987, 0.6953], q:[0.7682, 0.5365], qb:[0.4506, 0.3906], phi:[0.4635]] | 2*t^2.086 + t^2.524 + t^2.781 + t^2.961 + t^3.219 + t^3.476 + t^3.656 + t^3.734 + t^4.094 + 4*t^4.172 + t^4.352 + 3*t^4.609 + 2*t^4.867 + 3*t^5.047 + 3*t^5.305 + t^5.485 + 2*t^5.562 + 3*t^5.742 + t^5.82 + t^5.922 - t^6. - t^4.391/y - t^4.391*y | detail |