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 |
|---|---|---|---|---|---|---|---|---|---|
| 2365 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_1$ + $ M_5q_2\tilde{q}_2$ + $ M_6q_2\tilde{q}_1$ + $ M_4M_6$ + $ M_3^2$ + $ M_1M_5$ + $ M_4M_7$ | 0.6917 | 0.8492 | 0.8144 | [X:[], M:[1.0057, 0.9972, 1.0, 1.0113, 0.9943, 0.9887, 0.9887], q:[0.4858, 0.5085], qb:[0.5028, 0.4972], phi:[0.5014]] | [X:[], M:[[-4], [2], [0], [-8], [4], [8], [8]], q:[[10], [-6]], qb:[[-2], [2]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $q_1\tilde{q}_2$, $ M_6$, $ M_7$, $ M_5$, $ M_2$, $ M_3$, $ M_1$, $ \phi_1q_1^2$, $ \phi_1q_1\tilde{q}_2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1q_1q_2$, $ \phi_1\tilde{q}_2^2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_2\tilde{q}_2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_2^2$, $ q_1^2\tilde{q}_2^2$, $ M_6q_1\tilde{q}_2$, $ M_7q_1\tilde{q}_2$, $ M_6^2$, $ M_6M_7$, $ M_7^2$, $ M_5q_1\tilde{q}_2$, $ M_2q_1\tilde{q}_2$, $ M_5M_6$, $ M_5M_7$, $ M_2M_6$, $ M_2M_7$, $ M_2M_5$, $ M_5^2$, $ M_3M_6$, $ M_3M_7$, $ M_2^2$, $ M_3M_5$, $ M_1M_6$, $ M_1M_7$, $ M_2M_3$ | . | -2 | t^2.95 + 2*t^2.97 + t^2.98 + t^2.99 + t^3. + t^3.02 + t^4.42 + t^4.45 + t^4.47 + 2*t^4.49 + t^4.5 + 2*t^4.52 + t^4.54 + t^4.56 + t^5.9 + 2*t^5.91 + 3*t^5.93 + t^5.94 + 2*t^5.95 + 2*t^5.96 + 3*t^5.97 + t^5.98 + t^5.99 - 2*t^6. + t^6.01 - t^6.02 - t^6.03 - t^6.05 - t^6.07 + t^7.37 + 2*t^7.39 + 2*t^7.4 + 3*t^7.42 + 4*t^7.44 + 4*t^7.45 + 4*t^7.47 + 4*t^7.49 + 3*t^7.5 + 2*t^7.52 + t^7.54 + t^8.84 + t^8.85 + 2*t^8.86 + t^8.87 + 3*t^8.88 + 2*t^8.89 + 4*t^8.9 + 6*t^8.91 + 4*t^8.92 + t^8.93 + 5*t^8.94 - 2*t^8.95 + 4*t^8.96 - t^8.97 - 6*t^8.98 + t^8.99 - t^4.5/y - t^7.47/y + t^7.54/y + (2*t^8.91)/y + (2*t^8.93)/y + t^8.94/y + (3*t^8.95)/y + (2*t^8.96)/y + (4*t^8.97)/y + (3*t^8.98)/y + t^8.99/y - t^4.5*y - t^7.47*y + t^7.54*y + 2*t^8.91*y + 2*t^8.93*y + t^8.94*y + 3*t^8.95*y + 2*t^8.96*y + 4*t^8.97*y + 3*t^8.98*y + t^8.99*y | g1^12*t^2.95 + 2*g1^8*t^2.97 + g1^4*t^2.98 + g1^2*t^2.99 + t^3. + t^3.02/g1^4 + g1^19*t^4.42 + g1^11*t^4.45 + g1^7*t^4.47 + 2*g1^3*t^4.49 + t^4.5/g1 + (2*t^4.52)/g1^5 + t^4.54/g1^9 + t^4.56/g1^13 + g1^24*t^5.9 + 2*g1^20*t^5.91 + 3*g1^16*t^5.93 + g1^14*t^5.94 + 2*g1^12*t^5.95 + 2*g1^10*t^5.96 + g1^6*t^5.97 + 2*g1^8*t^5.97 + g1^4*t^5.98 + g1^2*t^5.99 - 2*t^6. + t^6.01/g1^2 - t^6.02/g1^4 - t^6.03/g1^8 - t^6.05/g1^12 - t^6.07/g1^16 + g1^31*t^7.37 + 2*g1^27*t^7.39 + 2*g1^23*t^7.4 + 3*g1^19*t^7.42 + 4*g1^15*t^7.44 + 4*g1^11*t^7.45 + 4*g1^7*t^7.47 + 4*g1^3*t^7.49 + (3*t^7.5)/g1 + (2*t^7.52)/g1^5 + t^7.54/g1^9 + g1^38*t^8.84 + g1^36*t^8.85 + 2*g1^32*t^8.86 + g1^30*t^8.87 + 3*g1^28*t^8.88 + 2*g1^26*t^8.89 + 4*g1^24*t^8.9 + 2*g1^20*t^8.91 + 4*g1^22*t^8.91 + 4*g1^18*t^8.92 + g1^16*t^8.93 + 5*g1^14*t^8.94 - 2*g1^12*t^8.95 + 4*g1^10*t^8.96 + 5*g1^6*t^8.97 - 6*g1^8*t^8.97 - 6*g1^4*t^8.98 + g1^2*t^8.99 - t^4.5/(g1*y) - (g1^7*t^7.47)/y + t^7.54/(g1^9*y) + (2*g1^20*t^8.91)/y + (2*g1^16*t^8.93)/y + (g1^14*t^8.94)/y + (3*g1^12*t^8.95)/y + (2*g1^10*t^8.96)/y + (g1^6*t^8.97)/y + (3*g1^8*t^8.97)/y + (3*g1^4*t^8.98)/y + (g1^2*t^8.99)/y - (t^4.5*y)/g1 - g1^7*t^7.47*y + (t^7.54*y)/g1^9 + 2*g1^20*t^8.91*y + 2*g1^16*t^8.93*y + g1^14*t^8.94*y + 3*g1^12*t^8.95*y + 2*g1^10*t^8.96*y + g1^6*t^8.97*y + 3*g1^8*t^8.97*y + 3*g1^4*t^8.98*y + g1^2*t^8.99*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 |
|---|---|---|---|---|---|---|---|---|
| 4360 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_1$ + $ M_5q_2\tilde{q}_2$ + $ M_6q_2\tilde{q}_1$ + $ M_4M_6$ + $ M_3^2$ + $ M_1M_5$ + $ M_4M_7$ + $ M_5M_8$ | 0.6914 | 0.8476 | 0.8157 | [X:[], M:[0.9996, 1.0002, 1.0, 0.9992, 1.0004, 1.0008, 1.0008, 0.9996], q:[0.501, 0.4994], qb:[0.4998, 0.5002], phi:[0.4999]] | 7*t^3. + 9*t^4.5 + t^4.51 + 8*t^6. - t^4.5/y - t^4.5*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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 1321 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2\phi_1^2$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_1\tilde{q}_1$ + $ M_5q_2\tilde{q}_2$ + $ M_6q_2\tilde{q}_1$ + $ M_4M_6$ + $ M_3^2$ + $ M_1M_5$ | 0.6917 | 0.8473 | 0.8164 | [X:[], M:[0.9935, 1.0033, 1.0, 0.9869, 1.0065, 1.0131], q:[0.5164, 0.4902], qb:[0.4967, 0.5033], phi:[0.4984]] | t^2.96 + t^2.98 + t^3. + t^3.01 + t^3.02 + t^3.04 + t^3.06 + t^4.44 + t^4.46 + 2*t^4.48 + t^4.5 + 2*t^4.51 + t^4.53 + t^4.55 + t^4.59 + t^5.97 + t^5.99 - t^6. - t^4.5/y - t^4.5*y | detail |