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 |
|---|---|---|---|---|---|---|---|---|---|
| 56043 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{4}M_{6}$ + ${ }M_{1}M_{5}$ + ${ }M_{7}\phi_{1}q_{1}q_{2}$ | 0.6505 | 0.8155 | 0.7976 | [M:[1.1798, 0.7192, 0.8202, 0.8539, 0.8202, 1.1461, 0.7865], q:[0.4269, 0.3933], qb:[0.8539, 0.7529], phi:[0.3933]] | [M:[[3], [12], [-3], [-8], [-3], [8], [2]], q:[[-4], [1]], qb:[[-8], [7]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{5}$, ${ }M_{6}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{6}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$ | ${}$ | -1 | t^2.158 + 2*t^2.36 + 2*t^2.461 + t^3.438 + t^3.539 + 2*t^3.741 + t^4.315 + 2*t^4.517 + 2*t^4.618 + 3*t^4.719 + 5*t^4.82 + 3*t^4.921 + t^5.596 + t^5.697 + t^5.798 + 4*t^5.899 - t^6. + 2*t^6.101 + 3*t^6.202 + t^6.473 + 2*t^6.675 + 2*t^6.776 + 4*t^6.877 + 5*t^6.978 + 5*t^7.079 + 6*t^7.18 + 5*t^7.281 + t^7.382 + 2*t^7.483 + t^7.754 + t^7.855 + t^7.956 + 4*t^8.057 + 3*t^8.259 - 3*t^8.461 + 2*t^8.562 + t^8.631 + 3*t^8.663 + 2*t^8.833 + 2*t^8.934 - t^4.18/y - t^6.337/y - (2*t^6.539)/y - t^6.64/y + (2*t^7.517)/y + (2*t^7.618)/y + (2*t^7.719)/y + (6*t^7.82)/y + t^7.921/y + t^8.022/y - t^8.495/y + t^8.596/y - t^8.697/y + t^8.798/y + (3*t^8.899)/y - t^4.18*y - t^6.337*y - 2*t^6.539*y - t^6.64*y + 2*t^7.517*y + 2*t^7.618*y + 2*t^7.719*y + 6*t^7.82*y + t^7.921*y + t^8.022*y - t^8.495*y + t^8.596*y - t^8.697*y + t^8.798*y + 3*t^8.899*y | g1^12*t^2.158 + 2*g1^2*t^2.36 + (2*t^2.461)/g1^3 + g1^8*t^3.438 + g1^3*t^3.539 + (2*t^3.741)/g1^7 + g1^24*t^4.315 + 2*g1^14*t^4.517 + 2*g1^9*t^4.618 + 3*g1^4*t^4.719 + (5*t^4.82)/g1 + (3*t^4.921)/g1^6 + g1^20*t^5.596 + g1^15*t^5.697 + g1^10*t^5.798 + 4*g1^5*t^5.899 - t^6. + (2*t^6.101)/g1^5 + (3*t^6.202)/g1^10 + g1^36*t^6.473 + 2*g1^26*t^6.675 + 2*g1^21*t^6.776 + 4*g1^16*t^6.877 + 5*g1^11*t^6.978 + 5*g1^6*t^7.079 + 6*g1*t^7.18 + (5*t^7.281)/g1^4 + t^7.382/g1^9 + (2*t^7.483)/g1^14 + g1^32*t^7.754 + g1^27*t^7.855 + g1^22*t^7.956 + 4*g1^17*t^8.057 + 3*g1^7*t^8.259 - (3*t^8.461)/g1^3 + (2*t^8.562)/g1^8 + g1^48*t^8.631 + (3*t^8.663)/g1^13 + 2*g1^38*t^8.833 + 2*g1^33*t^8.934 - (g1*t^4.18)/y - (g1^13*t^6.337)/y - (2*g1^3*t^6.539)/y - t^6.64/(g1^2*y) + (2*g1^14*t^7.517)/y + (2*g1^9*t^7.618)/y + (2*g1^4*t^7.719)/y + (6*t^7.82)/(g1*y) + t^7.921/(g1^6*y) + t^8.022/(g1^11*y) - (g1^25*t^8.495)/y + (g1^20*t^8.596)/y - (g1^15*t^8.697)/y + (g1^10*t^8.798)/y + (3*g1^5*t^8.899)/y - g1*t^4.18*y - g1^13*t^6.337*y - 2*g1^3*t^6.539*y - (t^6.64*y)/g1^2 + 2*g1^14*t^7.517*y + 2*g1^9*t^7.618*y + 2*g1^4*t^7.719*y + (6*t^7.82*y)/g1 + (t^7.921*y)/g1^6 + (t^8.022*y)/g1^11 - g1^25*t^8.495*y + g1^20*t^8.596*y - g1^15*t^8.697*y + g1^10*t^8.798*y + 3*g1^5*t^8.899*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 |
|---|
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 |
|---|
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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 50757 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{4}M_{6}$ + ${ }M_{1}M_{5}$ | 0.6332 | 0.7848 | 0.8069 | [M:[1.1817, 0.7266, 0.8183, 0.8489, 0.8183, 1.1511], q:[0.4245, 0.3939], qb:[0.8489, 0.7572], phi:[0.3939]] | t^2.18 + t^2.363 + 2*t^2.455 + t^3.453 + t^3.545 + t^3.637 + 2*t^3.728 + t^4.36 + t^4.543 + 2*t^4.635 + t^4.727 + 3*t^4.818 + 3*t^4.91 + t^5.633 + t^5.725 + t^5.817 + 3*t^5.908 - t^4.182/y - t^4.182*y | detail |