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 |
|---|---|---|---|---|---|---|---|---|---|
| 56548 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{4}M_{6}$ + ${ }M_{7}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6816 | 0.86 | 0.7926 | [M:[1.1588, 1.0729, 0.8412, 0.7812, 0.6953, 1.2188, 0.6953], q:[0.3906, 0.4506], qb:[0.5365, 0.7682], phi:[0.4635]] | [M:[[-5], [4], [5], [-12], [-3], [12], [-3]], q:[[-6], [11]], qb:[[2], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{7}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{1}$, ${ }M_{6}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{5}$, ${ }M_{1}M_{7}$, ${ }\phi_{1}^{4}$, ${ }M_{2}M_{3}$, ${ }M_{5}M_{6}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{5}\phi_{1}q_{1}^{2}$, ${ }M_{7}\phi_{1}q_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ | ${}$ | -1 | 2*t^2.086 + t^2.524 + t^2.781 + t^2.961 + t^3.219 + t^3.476 + t^3.656 + t^3.734 + t^4.094 + 4*t^4.172 + t^4.352 + 3*t^4.609 + 2*t^4.867 + 3*t^5.047 + 3*t^5.305 + t^5.485 + 2*t^5.562 + 3*t^5.742 + t^5.82 + t^5.922 - t^6. + 3*t^6.18 + 6*t^6.258 + 2*t^6.438 + t^6.515 + 2*t^6.618 + 5*t^6.695 + 2*t^6.875 + 3*t^6.953 + t^7.055 + 5*t^7.133 + 2*t^7.313 + 4*t^7.391 + t^7.468 + 3*t^7.571 + 2*t^7.648 + t^7.75 + 5*t^7.828 + 2*t^7.906 + 3*t^8.008 - 3*t^8.086 + t^8.188 + 5*t^8.266 + 8*t^8.344 + 2*t^8.446 + t^8.601 + 6*t^8.703 + 5*t^8.781 + t^8.883 + t^8.961 - t^4.391/y - (2*t^6.476)/y + t^7.172/y + (2*t^7.609)/y + (2*t^7.867)/y + (2*t^8.047)/y + (5*t^8.305)/y + t^8.485/y - t^8.562/y + (4*t^8.742)/y + (2*t^8.82)/y - t^4.391*y - 2*t^6.476*y + t^7.172*y + 2*t^7.609*y + 2*t^7.867*y + 2*t^8.047*y + 5*t^8.305*y + t^8.485*y - t^8.562*y + 4*t^8.742*y + 2*t^8.82*y | (2*t^2.086)/g1^3 + g1^5*t^2.524 + t^2.781/g1^4 + g1^13*t^2.961 + g1^4*t^3.219 + t^3.476/g1^5 + g1^12*t^3.656 + t^3.734/g1^14 + g1^20*t^4.094 + (4*t^4.172)/g1^6 + g1^11*t^4.352 + 3*g1^2*t^4.609 + (2*t^4.867)/g1^7 + 3*g1^10*t^5.047 + 3*g1*t^5.305 + g1^18*t^5.485 + (2*t^5.562)/g1^8 + 3*g1^9*t^5.742 + t^5.82/g1^17 + g1^26*t^5.922 - t^6. + 3*g1^17*t^6.18 + (6*t^6.258)/g1^9 + 2*g1^8*t^6.438 + t^6.515/g1^18 + 2*g1^25*t^6.618 + (5*t^6.695)/g1 + 2*g1^16*t^6.875 + (3*t^6.953)/g1^10 + g1^33*t^7.055 + 5*g1^7*t^7.133 + 2*g1^24*t^7.313 + (4*t^7.391)/g1^2 + t^7.468/g1^28 + 3*g1^15*t^7.571 + (2*t^7.648)/g1^11 + g1^32*t^7.75 + 5*g1^6*t^7.828 + (2*t^7.906)/g1^20 + 3*g1^23*t^8.008 - (3*t^8.086)/g1^3 + g1^40*t^8.188 + 5*g1^14*t^8.266 + (8*t^8.344)/g1^12 + 2*g1^31*t^8.446 + t^8.601/g1^21 + 6*g1^22*t^8.703 + (5*t^8.781)/g1^4 + g1^39*t^8.883 + g1^13*t^8.961 - t^4.391/(g1^2*y) - (2*t^6.476)/(g1^5*y) + t^7.172/(g1^6*y) + (2*g1^2*t^7.609)/y + (2*t^7.867)/(g1^7*y) + (2*g1^10*t^8.047)/y + (5*g1*t^8.305)/y + (g1^18*t^8.485)/y - t^8.562/(g1^8*y) + (4*g1^9*t^8.742)/y + (2*t^8.82)/(g1^17*y) - (t^4.391*y)/g1^2 - (2*t^6.476*y)/g1^5 + (t^7.172*y)/g1^6 + 2*g1^2*t^7.609*y + (2*t^7.867*y)/g1^7 + 2*g1^10*t^8.047*y + 5*g1*t^8.305*y + g1^18*t^8.485*y - (t^8.562*y)/g1^8 + 4*g1^9*t^8.742*y + (2*t^8.82*y)/g1^17 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 53796 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{4}M_{6}$ | 0.661 | 0.8205 | 0.8057 | [M:[1.1596, 1.0724, 0.8404, 0.7829, 0.6957, 1.2171], q:[0.3915, 0.449], qb:[0.5362, 0.7681], phi:[0.4638]] | t^2.087 + t^2.521 + t^2.783 + t^2.955 + t^3.217 + t^3.479 + t^3.651 + t^3.74 + t^3.913 + t^4.085 + 2*t^4.174 + t^4.347 + 2*t^4.609 + t^4.87 + 2*t^5.043 + 2*t^5.304 + t^5.477 + t^5.566 + 2*t^5.738 + t^5.911 - t^4.391/y - t^4.391*y | detail |