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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4349 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{5}X_{1}$ + ${ }M_{4}M_{7}$ + ${ }M_{8}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6883 | 0.8798 | 0.7823 | [X:[1.5103], M:[0.8513, 0.7872, 0.9154, 1.2128, 0.4897, 0.7231, 0.7872, 0.7872], q:[0.7872, 0.3615], qb:[0.4256, 0.7231], phi:[0.4256]] | [X:[[7]], M:[[-4], [1], [-9], [-1], [-7], [6], [1], [1]], q:[[1], [3]], qb:[[-2], [6]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{6}$, ${ }M_{2}$, ${ }M_{7}$, ${ }M_{8}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{6}M_{8}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{2}M_{8}$, ${ }M_{7}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{1}M_{8}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{7}$, ${ }M_{3}M_{8}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{7}\phi_{1}q_{2}^{2}$, ${ }M_{8}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{7}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{8}\tilde{q}_{1}\tilde{q}_{2}$ | ${}\phi_{1}^{3}q_{2}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0 | t^2.169 + 3*t^2.362 + 2*t^2.554 + t^2.746 + 2*t^3.446 + t^4.338 + 5*t^4.531 + 9*t^4.723 + 6*t^4.915 + 5*t^5.108 + 2*t^5.3 + t^5.492 + 3*t^5.615 + 5*t^5.808 - 2*t^6.192 - t^6.385 + t^6.508 + 5*t^6.7 + 14*t^6.892 + 16*t^7.085 + 12*t^7.277 + 12*t^7.469 + 9*t^7.662 + 3*t^7.785 + 5*t^7.854 + 9*t^7.977 + 2*t^8.046 + 7*t^8.169 + t^8.238 - 9*t^8.362 - 9*t^8.554 + t^8.677 - 8*t^8.746 + 5*t^8.869 - 4*t^8.938 - t^4.277/y - t^6.446/y - (2*t^6.638)/y - (2*t^6.831)/y - t^7.023/y + (4*t^7.531)/y + (7*t^7.723)/y + (9*t^7.915)/y + (5*t^8.108)/y + (2*t^8.3)/y + t^8.615/y + (4*t^8.808)/y - t^4.277*y - t^6.446*y - 2*t^6.638*y - 2*t^6.831*y - t^7.023*y + 4*t^7.531*y + 7*t^7.723*y + 9*t^7.915*y + 5*t^8.108*y + 2*t^8.3*y + t^8.615*y + 4*t^8.808*y | g1^6*t^2.169 + 3*g1*t^2.362 + (2*t^2.554)/g1^4 + t^2.746/g1^9 + 2*g1^4*t^3.446 + g1^12*t^4.338 + 5*g1^7*t^4.531 + 9*g1^2*t^4.723 + (6*t^4.915)/g1^3 + (5*t^5.108)/g1^8 + (2*t^5.3)/g1^13 + t^5.492/g1^18 + 3*g1^10*t^5.615 + 5*g1^5*t^5.808 - (2*t^6.192)/g1^5 - t^6.385/g1^10 + g1^18*t^6.508 + 5*g1^13*t^6.7 + 14*g1^8*t^6.892 + 16*g1^3*t^7.085 + (12*t^7.277)/g1^2 + (12*t^7.469)/g1^7 + (9*t^7.662)/g1^12 + 3*g1^16*t^7.785 + (5*t^7.854)/g1^17 + 9*g1^11*t^7.977 + (2*t^8.046)/g1^22 + 7*g1^6*t^8.169 + t^8.238/g1^27 - 9*g1*t^8.362 - (9*t^8.554)/g1^4 + g1^24*t^8.677 - (8*t^8.746)/g1^9 + 5*g1^19*t^8.869 - (4*t^8.938)/g1^14 - t^4.277/(g1^2*y) - (g1^4*t^6.446)/y - (2*t^6.638)/(g1*y) - (2*t^6.831)/(g1^6*y) - t^7.023/(g1^11*y) + (4*g1^7*t^7.531)/y + (7*g1^2*t^7.723)/y + (9*t^7.915)/(g1^3*y) + (5*t^8.108)/(g1^8*y) + (2*t^8.3)/(g1^13*y) + (g1^10*t^8.615)/y + (4*g1^5*t^8.808)/y - (t^4.277*y)/g1^2 - g1^4*t^6.446*y - (2*t^6.638*y)/g1 - (2*t^6.831*y)/g1^6 - (t^7.023*y)/g1^11 + 4*g1^7*t^7.531*y + 7*g1^2*t^7.723*y + (9*t^7.915*y)/g1^3 + (5*t^8.108*y)/g1^8 + (2*t^8.3*y)/g1^13 + g1^10*t^8.615*y + 4*g1^5*t^8.808*y |
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 |
---|---|---|---|---|---|---|---|---|---|
2353 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{5}X_{1}$ + ${ }M_{4}M_{7}$ | 0.6711 | 0.8492 | 0.7903 | [X:[1.5139], M:[0.8492, 0.7877, 0.9107, 1.2123, 0.4861, 0.7262, 0.7877], q:[0.7877, 0.3631], qb:[0.4246, 0.7262], phi:[0.4246]] | t^2.179 + 2*t^2.363 + 2*t^2.548 + t^2.732 + 2*t^3.452 + t^3.637 + t^4.357 + 4*t^4.542 + 6*t^4.726 + 4*t^4.911 + 4*t^5.095 + 2*t^5.28 + t^5.464 + 3*t^5.631 + 4*t^5.816 + 2*t^6. - t^4.274/y - t^4.274*y | detail |