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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2837 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}^{4}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ | 0.6791 | 0.8777 | 0.7737 | [M:[0.8226, 1.1774, 0.8226, 0.6774, 0.8226], q:[0.75, 0.4274], qb:[0.4274, 0.3951], phi:[0.5]] | [M:[[1], [-1], [1], [-1], [1]], q:[[0], [-1]], qb:[[-1], [2]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{4}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ | ${}M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ | -3 | t^2.032 + 4*t^2.468 + t^2.565 + t^3. + t^3.435 + t^3.871 + t^3.968 + 4*t^4.065 + 4*t^4.5 + t^4.597 + 10*t^4.935 + 5*t^5.032 + t^5.129 + 5*t^5.468 + t^5.565 + 3*t^5.903 - 3*t^6. + 2*t^6.097 + 4*t^6.338 + 4*t^6.435 + 13*t^6.532 + 4*t^6.629 + t^6.871 + 7*t^6.968 + 4*t^7.065 + t^7.162 + t^7.306 + 17*t^7.403 + 10*t^7.5 + t^7.597 + t^7.694 + t^7.741 + t^7.838 + 13*t^7.935 + 8*t^8.129 + 6*t^8.371 - 14*t^8.468 + t^8.565 + 2*t^8.662 + 10*t^8.806 + 9*t^8.903 - t^4.5/y - t^6.532/y - (2*t^6.968)/y + (4*t^7.5)/y + t^7.597/y + (6*t^7.935)/y + (7*t^8.032)/y + (6*t^8.468)/y + (5*t^8.903)/y - t^4.5*y - t^6.532*y - 2*t^6.968*y + 4*t^7.5*y + t^7.597*y + 6*t^7.935*y + 7*t^8.032*y + 6*t^8.468*y + 5*t^8.903*y | t^2.032/g1 + 4*g1*t^2.468 + t^2.565/g1^2 + t^3. + g1^2*t^3.435 + g1^4*t^3.871 + g1*t^3.968 + (4*t^4.065)/g1^2 + 4*t^4.5 + t^4.597/g1^3 + 10*g1^2*t^4.935 + (5*t^5.032)/g1 + t^5.129/g1^4 + 5*g1*t^5.468 + t^5.565/g1^2 + 3*g1^3*t^5.903 - 3*t^6. + (2*t^6.097)/g1^3 + 4*g1^5*t^6.338 + 4*g1^2*t^6.435 + (13*t^6.532)/g1 + (4*t^6.629)/g1^4 + g1^4*t^6.871 + 7*g1*t^6.968 + (4*t^7.065)/g1^2 + t^7.162/g1^5 + g1^6*t^7.306 + 17*g1^3*t^7.403 + 10*t^7.5 + t^7.597/g1^3 + t^7.694/g1^6 + g1^8*t^7.741 + g1^5*t^7.838 + 13*g1^2*t^7.935 + (8*t^8.129)/g1^4 + 6*g1^4*t^8.371 - 14*g1*t^8.468 + t^8.565/g1^2 + (2*t^8.662)/g1^5 + 10*g1^6*t^8.806 + 9*g1^3*t^8.903 - t^4.5/y - t^6.532/(g1*y) - (2*g1*t^6.968)/y + (4*t^7.5)/y + t^7.597/(g1^3*y) + (6*g1^2*t^7.935)/y + (7*t^8.032)/(g1*y) + (6*g1*t^8.468)/y + (5*g1^3*t^8.903)/y - t^4.5*y - (t^6.532*y)/g1 - 2*g1*t^6.968*y + 4*t^7.5*y + (t^7.597*y)/g1^3 + 6*g1^2*t^7.935*y + (7*t^8.032*y)/g1 + 6*g1*t^8.468*y + 5*g1^3*t^8.903*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 |
---|---|---|---|---|---|---|---|---|---|
1819 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}^{4}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ | 0.6643 | 0.8518 | 0.7799 | [M:[0.8278, 1.1722, 0.8278, 0.6722], q:[0.75, 0.4222], qb:[0.4222, 0.4056], phi:[0.5]] | t^2.017 + 3*t^2.483 + t^2.533 + t^3. + t^3.467 + t^3.517 + t^3.934 + t^3.983 + 4*t^4.033 + 3*t^4.5 + t^4.55 + 6*t^4.967 + 4*t^5.017 + t^5.066 + 4*t^5.483 + 2*t^5.533 + 2*t^5.95 - t^4.5/y - t^4.5*y | detail |