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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46964 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ | 0.6925 | 0.9093 | 0.7615 | [M:[0.8231, 0.7074, 0.6769, 0.6769, 1.1463], q:[0.75, 0.4269], qb:[0.3963, 0.4269], phi:[0.5]] | [M:[[-1], [4], [1], [1], [-2]], q:[[0], [1]], qb:[[-2], [1]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{3}$, ${ }M_{4}$, ${ }M_{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{4}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | ${}$ | -2 | 2*t^2.031 + t^2.122 + 3*t^2.469 + t^3. + 2*t^3.439 + t^3.531 + 6*t^4.061 + 2*t^4.153 + t^4.244 + 6*t^4.5 + 3*t^4.592 + 6*t^4.939 + 2*t^5.031 + t^5.122 + 7*t^5.469 + 4*t^5.561 + t^5.653 + 4*t^5.908 - 2*t^6. + 8*t^6.092 + 6*t^6.183 + 2*t^6.275 + t^6.367 + 15*t^6.531 + 6*t^6.622 + 3*t^6.714 + 2*t^6.878 + 10*t^6.969 + 9*t^7.061 + 2*t^7.153 + t^7.244 + 6*t^7.408 + 10*t^7.5 + 9*t^7.592 + 4*t^7.683 + t^7.775 + 10*t^7.939 - 4*t^8.031 + 13*t^8.122 + 8*t^8.214 + 6*t^8.306 + 6*t^8.378 + 2*t^8.397 - 9*t^8.469 + t^8.489 + 18*t^8.561 + 15*t^8.653 + 6*t^8.744 + 3*t^8.836 + 2*t^8.908 - t^4.5/y - (2*t^6.531)/y - t^6.622/y - t^6.969/y + (2*t^7.061)/y + (2*t^7.153)/y + (6*t^7.5)/y + (3*t^7.592)/y + (2*t^7.939)/y + (3*t^8.031)/y + t^8.122/y + t^8.378/y + (9*t^8.469)/y + t^8.561/y - t^8.653/y - t^8.744/y + (6*t^8.908)/y - t^4.5*y - 2*t^6.531*y - t^6.622*y - t^6.969*y + 2*t^7.061*y + 2*t^7.153*y + 6*t^7.5*y + 3*t^7.592*y + 2*t^7.939*y + 3*t^8.031*y + t^8.122*y + t^8.378*y + 9*t^8.469*y + t^8.561*y - t^8.653*y - t^8.744*y + 6*t^8.908*y | 2*g1*t^2.031 + g1^4*t^2.122 + (3*t^2.469)/g1 + t^3. + (2*t^3.439)/g1^2 + g1*t^3.531 + 6*g1^2*t^4.061 + 2*g1^5*t^4.153 + g1^8*t^4.244 + 6*t^4.5 + 3*g1^3*t^4.592 + (6*t^4.939)/g1^2 + 2*g1*t^5.031 + g1^4*t^5.122 + (7*t^5.469)/g1 + 4*g1^2*t^5.561 + g1^5*t^5.653 + (4*t^5.908)/g1^3 - 2*t^6. + 8*g1^3*t^6.092 + 6*g1^6*t^6.183 + 2*g1^9*t^6.275 + g1^12*t^6.367 + 15*g1*t^6.531 + 6*g1^4*t^6.622 + 3*g1^7*t^6.714 + (2*t^6.878)/g1^4 + (10*t^6.969)/g1 + 9*g1^2*t^7.061 + 2*g1^5*t^7.153 + g1^8*t^7.244 + (6*t^7.408)/g1^3 + 10*t^7.5 + 9*g1^3*t^7.592 + 4*g1^6*t^7.683 + g1^9*t^7.775 + (10*t^7.939)/g1^2 - 4*g1*t^8.031 + 13*g1^4*t^8.122 + 8*g1^7*t^8.214 + 6*g1^10*t^8.306 + (6*t^8.378)/g1^4 + 2*g1^13*t^8.397 - (9*t^8.469)/g1 + g1^16*t^8.489 + 18*g1^2*t^8.561 + 15*g1^5*t^8.653 + 6*g1^8*t^8.744 + 3*g1^11*t^8.836 + (2*t^8.908)/g1^3 - t^4.5/y - (2*g1*t^6.531)/y - (g1^4*t^6.622)/y - t^6.969/(g1*y) + (2*g1^2*t^7.061)/y + (2*g1^5*t^7.153)/y + (6*t^7.5)/y + (3*g1^3*t^7.592)/y + (2*t^7.939)/(g1^2*y) + (3*g1*t^8.031)/y + (g1^4*t^8.122)/y + t^8.378/(g1^4*y) + (9*t^8.469)/(g1*y) + (g1^2*t^8.561)/y - (g1^5*t^8.653)/y - (g1^8*t^8.744)/y + (6*t^8.908)/(g1^3*y) - t^4.5*y - 2*g1*t^6.531*y - g1^4*t^6.622*y - (t^6.969*y)/g1 + 2*g1^2*t^7.061*y + 2*g1^5*t^7.153*y + 6*t^7.5*y + 3*g1^3*t^7.592*y + (2*t^7.939*y)/g1^2 + 3*g1*t^8.031*y + g1^4*t^8.122*y + (t^8.378*y)/g1^4 + (9*t^8.469*y)/g1 + g1^2*t^8.561*y - g1^5*t^8.653*y - g1^8*t^8.744*y + (6*t^8.908*y)/g1^3 |
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 |
---|---|---|---|---|---|---|---|---|---|
46654 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.7058 | 0.934 | 0.7557 | [M:[0.8301, 0.6794, 0.6699, 0.6699], q:[0.75, 0.4199], qb:[0.4103, 0.4199], phi:[0.5]] | 2*t^2.01 + t^2.038 + 3*t^2.49 + t^2.519 + t^3. + t^3.481 + t^3.51 + 6*t^4.019 + 2*t^4.048 + t^4.076 + 6*t^4.5 + 5*t^4.529 + t^4.557 + 6*t^4.981 + 5*t^5.01 + 2*t^5.038 + 5*t^5.49 + 4*t^5.519 + t^5.548 + t^5.971 - t^6. - t^4.5/y - t^4.5*y | detail |