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 |
|---|---|---|---|---|---|---|---|---|---|
| 45349 | SO5adj1nf2 | $M_1q_1q_2$ + $ M_1\phi_1^2$ + $ M_2\phi_1^2$ + $ M_3q_1^2$ + $ M_4\phi_1^2q_1$ | 1.7538 | 1.8574 | 0.9442 | [X:[], M:[1.2, 1.2, 1.1611, 0.7806], q:[0.4194, 0.3806], qb:[], phi:[0.4]] | [X:[], M:[[0], [0], [2], [1]], q:[[-1], [1]], qb:[], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| $q_2^2$, $ M_4$, $ M_3$, $ \phi_1^2q_2$, $ M_1$, $ M_2$, $ \phi_1q_1q_2$, $ q_2^4$, $ M_4q_2^2$, $ M_4^2$, $ \phi_1^2q_2^2$, $ \phi_1^4$, $ \phi_1^2q_1q_2$, $ \phi_1^2q_1^2$, $ M_3q_2^2$, $ M_3M_4$, $ \phi_1^2q_2^3$, $ M_4\phi_1^2q_2$, $ M_2q_2^2$, $ \phi_1q_1q_2^3$, $ M_1M_4$, $ M_2M_4$, $ M_4\phi_1q_1q_2$ | $\phi_1^3q_1q_2$ | -1 | t^2.28 + t^2.34 + t^3.48 + t^3.54 + 3*t^3.6 + t^4.57 + t^4.63 + 2*t^4.68 + 2*t^4.8 + t^4.92 + t^5.77 + 2*t^5.83 + 3*t^5.88 + 3*t^5.94 - t^6. - t^6.12 + t^6.85 + t^6.91 + 3*t^6.97 + 3*t^7.03 + 5*t^7.08 + 4*t^7.14 + 5*t^7.2 - t^7.32 + t^8.05 + 2*t^8.11 + 5*t^8.17 + 4*t^8.23 + 5*t^8.28 + 4*t^8.4 - t^8.46 + t^8.52 - t^4.2/y - t^5.34/y - t^5.46/y - t^6.48/y - t^6.54/y - t^6.6/y - (2*t^7.68)/y - (2*t^7.74)/y - (3*t^7.8)/y + t^8.88/y - t^4.2*y - t^5.34*y - t^5.46*y - t^6.48*y - t^6.54*y - t^6.6*y - 2*t^7.68*y - 2*t^7.74*y - 3*t^7.8*y + t^8.88*y | g1^2*t^2.28 + g1*t^2.34 + g1^2*t^3.48 + g1*t^3.54 + 3*t^3.6 + g1^4*t^4.57 + g1^3*t^4.63 + 2*g1^2*t^4.68 + 2*t^4.8 + t^4.92/g1^2 + g1^4*t^5.77 + 2*g1^3*t^5.83 + 3*g1^2*t^5.88 + 3*g1*t^5.94 - t^6. - t^6.12/g1^2 + g1^6*t^6.85 + g1^5*t^6.91 + 3*g1^4*t^6.97 + 3*g1^3*t^7.03 + 5*g1^2*t^7.08 + 4*g1*t^7.14 + 5*t^7.2 - t^7.32/g1^2 + g1^6*t^8.05 + 2*g1^5*t^8.11 + 5*g1^4*t^8.17 + 4*g1^3*t^8.23 + 5*g1^2*t^8.28 + 4*t^8.4 - t^8.46/g1 + t^8.52/g1^2 - t^4.2/y - (g1*t^5.34)/y - t^5.46/(g1*y) - (g1^2*t^6.48)/y - (g1*t^6.54)/y - t^6.6/y - (2*g1^2*t^7.68)/y - (2*g1*t^7.74)/y - (3*t^7.8)/y + (g1^2*t^8.88)/y - t^4.2*y - g1*t^5.34*y - (t^5.46*y)/g1 - g1^2*t^6.48*y - g1*t^6.54*y - t^6.6*y - 2*g1^2*t^7.68*y - 2*g1*t^7.74*y - 3*t^7.8*y + g1^2*t^8.88*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 |
|---|---|---|---|---|---|---|---|---|---|
| 45166 | SO5adj1nf2 | $M_1q_1q_2$ + $ M_1\phi_1^2$ + $ M_2\phi_1^2$ + $ M_3q_1^2$ | 1.7363 | 1.8255 | 0.9511 | [X:[], M:[1.2, 1.2, 1.1729], q:[0.4135, 0.3865], qb:[], phi:[0.4]] | t^2.32 + t^3.52 + t^3.56 + 3*t^3.6 + t^3.64 + t^4.64 + t^4.72 + 2*t^4.8 + t^4.88 + t^5.84 + t^5.88 + 2*t^5.92 + t^5.96 - t^6. - t^4.2/y - t^5.36/y - t^5.44/y - t^4.2*y - t^5.36*y - t^5.44*y | detail |