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 |
|---|---|---|---|---|---|---|---|---|---|
| 46102 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_3q_1\tilde{q}_2$ + $ M_3^2$ + $ q_2^2\tilde{q}_1\tilde{q}_2$ + $ M_1X_1$ | 0.599 | 0.7629 | 0.7852 | [X:[1.3787], M:[0.6213, 0.6765, 1.0], q:[0.7702, 0.6085], qb:[0.5533, 0.2298], phi:[0.4596]] | [X:[[6]], M:[[-6], [16], [0]], q:[[-1], [7]], qb:[[-15], [1]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $M_2$, $ \tilde{q}_1\tilde{q}_2$, $ q_2\tilde{q}_2$, $ \phi_1^2$, $ \phi_1\tilde{q}_2^2$, $ M_3$, $ q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2$, $ M_2^2$, $ X_1$, $ \phi_1q_1\tilde{q}_2$, $ M_2\tilde{q}_1\tilde{q}_2$, $ M_2q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1^2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ M_2\phi_1^2$, $ M_2\phi_1\tilde{q}_2^2$, $ \phi_1q_2\tilde{q}_1$, $ q_2\tilde{q}_1\tilde{q}_2^2$, $ M_2M_3$, $ \phi_1q_2^2$, $ q_2^2\tilde{q}_2^2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2^3$, $ \phi_1^2q_2\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2^3$, $ \phi_1q_1\tilde{q}_1$, $ M_3\tilde{q}_1\tilde{q}_2$, $ \phi_1^4$, $ \phi_1q_1q_2$, $ M_2q_2\tilde{q}_1$, $ M_3q_2\tilde{q}_2$, $ \phi_1^3\tilde{q}_2^2$, $ \phi_1^2\tilde{q}_2^4$, $ M_3\phi_1^2$, $ M_2\phi_1\tilde{q}_1\tilde{q}_2$, $ M_3\phi_1\tilde{q}_2^2$, $ M_2\phi_1q_2\tilde{q}_2$ | . | -2 | t^2.03 + t^2.35 + t^2.51 + 2*t^2.76 + t^3. + t^3.49 + t^3.73 + t^3.89 + t^4.06 + t^4.14 + t^4.38 + t^4.54 + 2*t^4.7 + 2*t^4.79 + t^4.86 + 2*t^5.03 + 2*t^5.11 + 2*t^5.27 + t^5.35 + 5*t^5.51 + 2*t^5.76 + t^5.92 - 2*t^6. + t^6.08 + t^6.09 + 2*t^6.24 + t^6.41 + 2*t^6.49 + t^6.57 + 2*t^6.65 + t^6.73 + 2*t^6.82 + 2*t^6.89 - t^6.97 + 2*t^7.05 + 2*t^7.06 + t^7.14 + t^7.21 + 2*t^7.3 + 4*t^7.46 + 5*t^7.54 + t^7.62 + t^7.7 + 4*t^7.79 + 3*t^7.86 - t^7.94 + t^7.95 + 2*t^8.03 + t^8.11 + t^8.12 + t^8.18 + 7*t^8.27 - 3*t^8.35 + 2*t^8.43 + t^8.44 + t^8.6 + 2*t^8.68 - 5*t^8.76 + 2*t^8.83 + 2*t^8.85 + t^8.92 - t^4.38/y - t^6.41/y - t^7.14/y + t^7.38/y + t^7.54/y + t^7.62/y + (2*t^7.79)/y + t^7.86/y + t^8.03/y + (2*t^8.11)/y + (2*t^8.27)/y + (2*t^8.35)/y - t^8.44/y + (3*t^8.51)/y + (3*t^8.76)/y + t^8.83/y + t^8.92/y - t^4.38*y - t^6.41*y - t^7.14*y + t^7.38*y + t^7.54*y + t^7.62*y + 2*t^7.79*y + t^7.86*y + t^8.03*y + 2*t^8.11*y + 2*t^8.27*y + 2*t^8.35*y - t^8.44*y + 3*t^8.51*y + 3*t^8.76*y + t^8.83*y + t^8.92*y | g1^16*t^2.03 + t^2.35/g1^14 + g1^8*t^2.51 + 2*g1^4*t^2.76 + t^3. + t^3.49/g1^8 + t^3.73/g1^12 + g1^10*t^3.89 + g1^32*t^4.06 + g1^6*t^4.14 + g1^2*t^4.38 + g1^24*t^4.54 + (2*t^4.7)/g1^28 + 2*g1^20*t^4.79 + t^4.86/g1^6 + 2*g1^16*t^5.03 + (2*t^5.11)/g1^10 + 2*g1^12*t^5.27 + t^5.35/g1^14 + 5*g1^8*t^5.51 + 2*g1^4*t^5.76 + g1^26*t^5.92 - 2*t^6. + t^6.08/g1^26 + g1^48*t^6.09 + (2*t^6.24)/g1^4 + g1^18*t^6.41 + (2*t^6.49)/g1^8 + g1^40*t^6.57 + 2*g1^14*t^6.65 + t^6.73/g1^12 + 2*g1^36*t^6.82 + 2*g1^10*t^6.89 - t^6.97/g1^16 + (2*t^7.05)/g1^42 + 2*g1^32*t^7.06 + g1^6*t^7.14 + t^7.21/g1^20 + 2*g1^28*t^7.3 + (4*t^7.46)/g1^24 + 5*g1^24*t^7.54 + t^7.62/g1^2 + t^7.7/g1^28 + 4*g1^20*t^7.79 + (3*t^7.86)/g1^6 - t^7.94/g1^32 + g1^42*t^7.95 + 2*g1^16*t^8.03 + t^8.11/g1^10 + g1^64*t^8.12 + t^8.18/g1^36 + 7*g1^12*t^8.27 - (3*t^8.35)/g1^14 + (2*t^8.43)/g1^40 + g1^34*t^8.44 + g1^56*t^8.6 + 2*g1^30*t^8.68 - 5*g1^4*t^8.76 + (2*t^8.83)/g1^22 + 2*g1^52*t^8.85 + g1^26*t^8.92 - (g1^2*t^4.38)/y - (g1^18*t^6.41)/y - (g1^6*t^7.14)/y + (g1^2*t^7.38)/y + (g1^24*t^7.54)/y + t^7.62/(g1^2*y) + (2*g1^20*t^7.79)/y + t^7.86/(g1^6*y) + (g1^16*t^8.03)/y + (2*t^8.11)/(g1^10*y) + (2*g1^12*t^8.27)/y + (2*t^8.35)/(g1^14*y) - (g1^34*t^8.44)/y + (3*g1^8*t^8.51)/y + (3*g1^4*t^8.76)/y + t^8.83/(g1^22*y) + (g1^26*t^8.92)/y - g1^2*t^4.38*y - g1^18*t^6.41*y - g1^6*t^7.14*y + g1^2*t^7.38*y + g1^24*t^7.54*y + (t^7.62*y)/g1^2 + 2*g1^20*t^7.79*y + (t^7.86*y)/g1^6 + g1^16*t^8.03*y + (2*t^8.11*y)/g1^10 + 2*g1^12*t^8.27*y + (2*t^8.35*y)/g1^14 - g1^34*t^8.44*y + 3*g1^8*t^8.51*y + 3*g1^4*t^8.76*y + (t^8.83*y)/g1^22 + g1^26*t^8.92*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 |
|---|---|---|---|---|---|---|---|---|
| 46730 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_3q_1\tilde{q}_2$ + $ M_3^2$ + $ q_2^2\tilde{q}_1\tilde{q}_2$ + $ M_1X_1$ + $ M_2M_4$ | 0.5782 | 0.722 | 0.8009 | [X:[1.3799], M:[0.6201, 0.6798, 1.0, 1.3202], q:[0.77, 0.6099], qb:[0.5501, 0.23], phi:[0.46]] | t^2.34 + t^2.52 + 2*t^2.76 + t^3. + t^3.48 + t^3.72 + t^3.9 + t^3.96 + t^4.14 + 2*t^4.68 + t^4.86 + t^5.04 + 2*t^5.1 + 2*t^5.28 + t^5.34 + 4*t^5.52 + t^5.76 - 2*t^6. - t^4.38/y - t^4.38*y | detail | |
| 46609 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_3q_1\tilde{q}_2$ + $ M_3^2$ + $ q_2^2\tilde{q}_1\tilde{q}_2$ + $ M_1X_1$ + $ M_4\phi_1\tilde{q}_1\tilde{q}_2$ + $ M_2X_2$ | 0.5972 | 0.7561 | 0.7898 | [X:[1.3731, 1.3384], M:[0.6269, 0.6616, 1.0, 0.7462], q:[0.7712, 0.6019], qb:[0.5673, 0.2288], phi:[0.4577]] | t^2.24 + t^2.39 + t^2.49 + 2*t^2.75 + t^3. + t^3.51 + t^3.87 + t^4.02 + t^4.12 + t^4.48 + t^4.63 + t^4.73 + 2*t^4.78 + t^4.88 + 3*t^4.98 + 2*t^5.13 + 3*t^5.24 + t^5.39 + 4*t^5.49 + 2*t^5.75 - 2*t^6. - t^4.37/y - t^4.37*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46026 | SU2adj1nf2 | $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ \phi_1q_1^2$ + $ M_3q_1\tilde{q}_2$ + $ M_3^2$ | 0.6271 | 0.8146 | 0.7698 | [X:[], M:[0.7084, 0.7084, 1.0], q:[0.7583, 0.5333], qb:[0.5333, 0.2417], phi:[0.4834]] | 2*t^2.13 + 2*t^2.32 + 2*t^2.9 + t^3. + t^3.2 + 2*t^3.77 + 3*t^4.25 + 4*t^4.45 + 6*t^4.65 + 4*t^5.03 + 4*t^5.23 + 4*t^5.32 + 2*t^5.52 + 3*t^5.8 + 5*t^5.9 - 5*t^6. - t^4.45/y - t^4.45*y | detail |