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 |
---|---|---|---|---|---|---|---|---|---|
57581 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ | 1.1267 | 1.3165 | 0.8559 | [X:[1.3575], M:[], q:[0.9819, 0.3394], qb:[0.3394, 0.3031], phi:[0.3394]] | [X:[[4]], M:[], q:[[-3], [1]], qb:[[1], [-5]], phi:[[1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{5}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${2}\phi_{1}^{4}q_{2}\tilde{q}_{2}$, ${ 2}\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ 2}\phi_{1}^{3}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 5 | 2*t^2.04 + t^2.95 + 2*t^3.05 + 2*t^3.85 + 3*t^3.96 + 4*t^4.07 + 2*t^4.87 + 3*t^4.98 + 3*t^5.09 + t^5.78 + 5*t^5.89 + 5*t^6. + 8*t^6.11 + 2*t^6.8 + 6*t^6.91 + 8*t^7.02 + 5*t^7.13 + 3*t^7.71 + 7*t^7.82 + 13*t^7.93 + 8*t^8.04 + 10*t^8.15 + 4*t^8.73 + 9*t^8.84 + 6*t^8.95 - t^4.02/y - t^5.04/y - (2*t^6.05)/y - (2*t^7.07)/y - t^7.87/y + t^7.98/y - t^8.09/y + (3*t^8.89)/y - t^4.02*y - t^5.04*y - 2*t^6.05*y - 2*t^7.07*y - t^7.87*y + t^7.98*y - t^8.09*y + 3*t^8.89*y | 2*g1^2*t^2.04 + t^2.95/g1^3 + 2*g1^3*t^3.05 + (2*t^3.85)/g1^8 + (3*t^3.96)/g1^2 + 4*g1^4*t^4.07 + (2*t^4.87)/g1^7 + (3*t^4.98)/g1 + 3*g1^5*t^5.09 + t^5.78/g1^12 + (5*t^5.89)/g1^6 + 5*t^6. + 8*g1^6*t^6.11 + (2*t^6.8)/g1^11 + (6*t^6.91)/g1^5 + 8*g1*t^7.02 + 5*g1^7*t^7.13 + (3*t^7.71)/g1^16 + (7*t^7.82)/g1^10 + (13*t^7.93)/g1^4 + 8*g1^2*t^8.04 + 10*g1^8*t^8.15 + (4*t^8.73)/g1^15 + (9*t^8.84)/g1^9 + (6*t^8.95)/g1^3 - (g1*t^4.02)/y - (g1^2*t^5.04)/y - (2*g1^3*t^6.05)/y - (2*g1^4*t^7.07)/y - t^7.87/(g1^7*y) + t^7.98/(g1*y) - (g1^5*t^8.09)/y + (3*t^8.89)/(g1^6*y) - g1*t^4.02*y - g1^2*t^5.04*y - 2*g1^3*t^6.05*y - 2*g1^4*t^7.07*y - (t^7.87*y)/g1^7 + (t^7.98*y)/g1 - g1^5*t^8.09*y + (3*t^8.89*y)/g1^6 |
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 |
---|---|---|---|---|---|---|---|---|
58567 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.1475 | 1.3573 | 0.8454 | [X:[1.357], M:[0.6785], q:[0.9823, 0.3392], qb:[0.3392, 0.3038], phi:[0.3392]] | 3*t^2.04 + t^2.95 + 2*t^3.05 + 2*t^3.86 + 2*t^3.96 + 7*t^4.07 + 2*t^4.88 + 4*t^4.98 + 5*t^5.09 + t^5.79 + 7*t^5.89 + 5*t^6. - t^4.02/y - t^5.04/y - t^4.02*y - t^5.04*y | detail | |
58719 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ | 1.1471 | 1.3549 | 0.8466 | [X:[1.3511], M:[0.7022], q:[0.9867, 0.3378], qb:[0.3378, 0.3111], phi:[0.3378]] | 2*t^2.03 + t^2.11 + t^2.96 + 2*t^3.04 + t^3.89 + 3*t^3.97 + 4*t^4.05 + 2*t^4.13 + t^4.21 + 2*t^4.91 + 3*t^4.99 + 4*t^5.07 + 2*t^5.15 + t^5.84 + 3*t^5.92 + 6*t^6. - t^4.01/y - t^5.03/y - t^4.01*y - t^5.03*y | detail |
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 |
---|---|---|---|---|---|---|---|---|---|
47925 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ | 1.2241 | 1.4234 | 0.86 | [X:[1.459], q:[0.7527, 0.2117], qb:[0.5178, 0.3292], phi:[0.3648]] | 2*t^2.189 + t^2.717 + t^3.246 + 2*t^3.283 + 2*t^3.811 + t^4.34 + 4*t^4.377 + 2*t^4.623 + 3*t^4.906 + 2*t^5.189 + 3*t^5.434 + 3*t^5.471 + 2*t^5.717 + t^5.963 + 3*t^6. - t^4.094/y - t^5.189/y - t^4.094*y - t^5.189*y | detail |