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 |
|---|---|---|---|---|---|---|---|---|---|
| 1988 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ | 0.6659 | 0.842 | 0.7909 | [M:[0.8176, 0.7588, 1.1824, 0.847, 0.7882, 0.7588], q:[0.8029, 0.8029], qb:[0.3794, 0.4382], phi:[0.3941]] | [M:[[6], [-14], [-6], [16], [-4], [-14]], q:[[1], [1]], qb:[[-7], [13]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{6}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{4}$, ${ }M_{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }q_{1}q_{2}$, ${ }M_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{6}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{6}q_{1}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{1}$ | ${}$ | -1 | 2*t^2.277 + 2*t^2.365 + t^2.453 + t^2.541 + 2*t^3.547 + t^3.812 + 3*t^4.553 + 4*t^4.641 + 5*t^4.729 + 5*t^4.818 + 3*t^4.906 + t^4.994 + t^5.082 + 3*t^5.824 + 2*t^5.912 - t^6. + 2*t^6.088 + t^6.176 + t^6.265 + t^6.353 + 4*t^6.83 + 6*t^6.918 + 8*t^7.006 + 13*t^7.094 + 7*t^7.182 + 3*t^7.271 + 5*t^7.359 + 2*t^7.447 + t^7.535 + 2*t^7.623 + 4*t^8.1 + 2*t^8.188 - 2*t^8.277 - t^8.365 - 3*t^8.453 - 2*t^8.541 + 3*t^8.629 + 2*t^8.717 + t^8.806 + t^8.894 - t^4.182/y - (2*t^6.459)/y - (2*t^6.547)/y - t^6.723/y + t^7.553/y + (5*t^7.641)/y + (3*t^7.729)/y + (6*t^7.818)/y + (4*t^7.906)/y + t^7.994/y - (3*t^8.735)/y + t^8.912/y - t^4.182*y - 2*t^6.459*y - 2*t^6.547*y - t^6.723*y + t^7.553*y + 5*t^7.641*y + 3*t^7.729*y + 6*t^7.818*y + 4*t^7.906*y + t^7.994*y - 3*t^8.735*y + t^8.912*y | (2*t^2.277)/g1^14 + (2*t^2.365)/g1^4 + g1^6*t^2.453 + g1^16*t^2.541 + (2*t^3.547)/g1^6 + g1^24*t^3.812 + (3*t^4.553)/g1^28 + (4*t^4.641)/g1^18 + (5*t^4.729)/g1^8 + 5*g1^2*t^4.818 + 3*g1^12*t^4.906 + g1^22*t^4.994 + g1^32*t^5.082 + (3*t^5.824)/g1^20 + (2*t^5.912)/g1^10 - t^6. + 2*g1^10*t^6.088 + g1^20*t^6.176 + g1^30*t^6.265 + g1^40*t^6.353 + (4*t^6.83)/g1^42 + (6*t^6.918)/g1^32 + (8*t^7.006)/g1^22 + (13*t^7.094)/g1^12 + (7*t^7.182)/g1^2 + 3*g1^8*t^7.271 + 5*g1^18*t^7.359 + 2*g1^28*t^7.447 + g1^38*t^7.535 + 2*g1^48*t^7.623 + (4*t^8.1)/g1^34 + (2*t^8.188)/g1^24 - (2*t^8.277)/g1^14 - t^8.365/g1^4 - 3*g1^6*t^8.453 - 2*g1^16*t^8.541 + 3*g1^26*t^8.629 + 2*g1^36*t^8.717 + g1^46*t^8.806 + g1^56*t^8.894 - t^4.182/(g1^2*y) - (2*t^6.459)/(g1^16*y) - (2*t^6.547)/(g1^6*y) - (g1^14*t^6.723)/y + t^7.553/(g1^28*y) + (5*t^7.641)/(g1^18*y) + (3*t^7.729)/(g1^8*y) + (6*g1^2*t^7.818)/y + (4*g1^12*t^7.906)/y + (g1^22*t^7.994)/y - (3*t^8.735)/(g1^30*y) + t^8.912/(g1^10*y) - (t^4.182*y)/g1^2 - (2*t^6.459*y)/g1^16 - (2*t^6.547*y)/g1^6 - g1^14*t^6.723*y + (t^7.553*y)/g1^28 + (5*t^7.641*y)/g1^18 + (3*t^7.729*y)/g1^8 + 6*g1^2*t^7.818*y + 4*g1^12*t^7.906*y + g1^22*t^7.994*y - (3*t^8.735*y)/g1^30 + (t^8.912*y)/g1^10 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 742 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6476 | 0.8091 | 0.8003 | [M:[0.8113, 0.7736, 1.1887, 0.8301, 0.7925], q:[0.8019, 0.8019], qb:[0.3868, 0.4245], phi:[0.3962]] | t^2.321 + 2*t^2.377 + t^2.434 + t^2.49 + 2*t^3.566 + t^3.679 + t^3.736 + t^4.642 + 2*t^4.698 + 4*t^4.755 + 4*t^4.811 + 3*t^4.868 + t^4.924 + t^4.981 + t^5.887 + 2*t^5.943 - t^4.189/y - t^4.189*y | detail |